Loudspeaker enclosure system with signal processor for enhanced perception of low frequency output

ABSTRACT

A loudspeaker system with a transducer and an enclosure with at least one resonant chamber, including a resonant-chamber resonance frequency, at which a displacement characteristic of a vibratile diaphragm of the transducer has a minimum. The loudspeaker system further includes a multi-mode signal processor with a set of signal processes wherein in one example, a variable gain, frequency selective dynamic filter reduces the gain in a high displacement frequency range upon an output in the frequency range exceeding an overload amplitude threshold. The gain reduction is compensated for by complimentary frequency generating signal processes, including at least one of a harmonics generator and a transpositional gain controller, with the signal processor adapted to match the resonant chamber enclosure by substantially maintaining or increasing acoustic output at the resonant chamber resonance and generating harmonics associated with fundamental frequencies in the gain reduced frequency range to maintain a perception of tonal quality and physical bass impact, increasing low frequency capability while minimizing audible overload distortion.

RELATED APPLICATIONS

This application, U.S. patent application Ser. No. 14/276,881 filed May 13, 2014, claims benefit of U.S. Provisional Application Ser. No. 61/823,356 filed May 14, 2013, the contents of which are incorporated herein by reference.

TECHNICAL FIELD

This invention is in the category of audio loudspeaker systems, more specifically, loudspeaker systems with signal processing for the purpose of enhancing low frequency capability.

BACKGROUND AND RELATED ART

In the audio field it has always been desirable for audio systems to be made smaller and lower cost, while at the same time producing the low frequency performance of a larger, higher cost system. This is also a goal in miniature devices, such as cell phones, tablet computers, and small multi-media loudspeakers systems. Similarly, even in larger systems, increased low frequency performance has been desired, such as in the professional, large venue loudspeaker system category, where systems are run at their full capability, singular systems that could achieve the low frequency capability in one loudspeaker enclosure that could duplicate that of two or more loudspeakers systems would be desirable. Additionally, increased low frequency capability has applications in all forms of audio reproduction that includes a low frequency range, including automotive systems, domestic audio systems, consumer audio devices, TV sound systems, home theater and surround sound systems, and music reproduction systems of all types.

A number of technologies have been suggested, each of which provide an enhancement to some aspect of lower frequencies in loudspeaker systems, but each prior art approach also comes with distinct perceptual shortcomings that in the final evaluation makes for a perceptually unconvincing alternative to a larger loudspeaker system.

Bass reproduction has two primary perceptual attributes that need to be satisfied in a small system if it is to convincingly replicate the perceived bass capability of a larger system; 1) tonal balance quality, and 2) physical impact, body-felt, quantity. And to match the capability of a larger system, both of these attributes must be achieved without audible overload distortion.

One approach of the prior art is that of systems that incorporate dynamic equalization, with the earliest of this type being U.S. Pat. No. 4,113,983, “INPUT FILTERING APPARATUS FOR LOUDSPEAKERS”, by Paul Steel, followed by later systems, such as U.S. Pat. No. 4,327,250 “DYNAMIC SPEAKER EQUALIZER”, by Daniel von Recklinghausen, U.S. Pat. No. 5,481,617, “LOUDSPEAKER ARRANGEMENT WITH FREQUENCY DEPENDENT AMPLITUDE REGULATIONS” by Egon Bjerre, U.S. Pat. No. 5,548,650 “SPEAKER EXCURSION CONTROL” by David Clarke, and U.S. Pat. No. 5,577,126, “Overload Protection Circuit for Transducers”, by Wolfgang Klippel, all of the same basic concept but with various processor control architectures.

These low frequency dynamic equalization systems basically equalize and extend low frequencies to allow a small loudspeaker to reproduce lower bass tones more accurately at small signal levels, but at larger signal levels, the majority of low frequencies are suppressed to avoid overload distortion from the low frequency woofer transducer, which also suppresses low frequency aural bass tonal level, and also, physical bass impact, at these larger signal levels, creating a thin sounding loudspeaker with substantially reduced bass impact, with very poor perceptual bass accuracy at all but very small signal levels. The bass is removed, and nothing is done to make up for, or correct the perception of poor bass reproduction at larger signal levels.

US Patent Application 2005/0207584, “SYSTEM FOR LIMITING LOUDSPEAKER DISPLACEMENT” by Andrew Bright, is another dynamic equalizer with additional signal processing, including digital implementation of the dynamic equalization. This system ultimately still suffers from similar limitations of other dynamic equalization processors reduction of physical bass impact and tonal balance quality at large signal levels without a means to correct these shortcomings.

Another approach is U.S. Patent Application 2004/0022400 “BASS COMPRESSOR” by Anthony Magrath, which uses a compressor as a ‘hard-clipper’, to limit bass and to use the distortion from the compressor such that the resultant distortion is heard as an increase in bass. This approach is problematic in that synthetic bass created by distortion has limited independent control. The requirements for optimal symmetry for compression/clipping and distortion based enhancement of low frequencies can be in conflict without isolated control, limiting the ability to independently allow the creation of an audible perceived bass response faithful to the original program source or desired bass tone increase. Also, the original physical bass impact is reduced when the compressor is activated. The application of Minnaar, “METHOD AND DEVICE FOR EXTENSION OF LOW FREQUENCY OUTPUT FROM A LOUDSPEAKER”, U.S. Patent Application 2010/0215192, is essentially a device similar in concept to Magrath but with an alternative control scheme.

Another approach to simulating greater performance from a smaller, lower powered, sound system is that of systems deploying the psychoacoustic effect of fundamental tracking or virtual pitch. An example of this type of system is typified in U.S. Pat. No. 5,668,885, “LOW FREQUENCY AUDIO CONVERSION CIRCUIT” by Mikio Oda. In these systems, a low frequency range is either inherently attenuated, or substantially removed by a static high pass filter, and an attempt is made to fill in a perception of the fundamental frequencies that were removed, by introducing harmonics of those now-missing bass frequencies, in the upper bass and lower midrange frequencies that can be more easily reproduced by the small loudspeaker and woofer transducer. The harmonics are generated statically, at all signal levels. While this can to some degree replace the bass “tones” over a narrow range of frequencies, it does not replace any of the physical bass impact of the bass, and it often applied over too wide of a frequency range to even accurately replace the tonal aspects for all the bass frequencies that are filtered out, resulting in both a total loss of physical bass impact and incomplete, or compromised, tonal quality. U.S. Pat. No. 5,930,373, “METHOD AND SYSTEM FOR ENHANCING QUALITY OF SOUND SIGNAL”, by Meir Shashoua, et al is based in the same concept of attempting to replace the tonal loss from a loudspeaker system with attenuated low frequency response, but similarly does nothing to compensate for loss of low frequency physical impact and because the artificial bass is used at small signal levels and large signal levels, it can impart an unrealistic coloration to the bass tone at all levels. Additional disclosures of this type of system are provided by Gan and Hawksford in “Perceptually-Motivated Objective Grading of Nonlinear Processing in Virtual-Bass Systems”, published in the Audio Engineering Society Journal, November 2011.

Prior art U.S. Patent Application 2007/0098182 “AUDIO FREQUENCY RANGE ADAPTATION” by R. M. Aarts, and in “High-Efficiency Low-BL Loudspeakers”, also by R. M. Aarts in the Audio Engineering Society Journal, July/August 2005, in order to reduce the size of a low frequency loudspeaker, uses a separate subwoofer box optimized to be efficient at one frequency, and uses a mapping processor to map the output of all bass frequencies below approximately 120 Hz to the one frequency. The subwoofer essentially plays just one frequency to replace all bass frequencies below 120 Hz, and this approach is applied statically at all signal levels. Because, in this system, for all bass frequencies there is only one frequency that is being reproduced, the audible output created has an unnatural bass tonal quality for all audio bass frequencies, at all signal levels. This is another system that creates a significant vacancy of frequencies throughout the bass range, with a perceptual “one note” bass effect, and it fails to recreate a realistic facsimile of a high quality low frequency system, and is relegated to use in low fidelity systems.

A common enclosure design is a sealed, acoustic suspension enclosure which exhibits increased diaphragm displacement throughout the lower frequencies without any resonant chamber based frequency and range of reduced diaphragm displacement, and tend to be a poor performer for low frequency acoustic output relative to diaphragm displacement. Historically vented box loudspeakers have been known to provide greater output at a vented box tuning frequency, for a given diaphragm displacement, but exhibit significantly greater diaphragm displacement for all frequencies below the tuning frequency and also for a band of frequencies above the tuning frequency, and therefore are limited in the ability to take advantage of the reduced diaphragm displacement at the vented box tuning to produce greater output over the full range of bass frequencies. These systems are disclosed in “Vented-Box Loudspeaker Systems Part 1 and Part 2”, in the Journal of the Audio Engineering Society, June and July/August 1973 issues, by Richard H. Small.

Single and multi-tuned bandpass enclosures attempt to improve output capability but still suffer from increased diaphragm displacement above the lowest tuning frequency, thereby limiting total output capability to the weakest, high displacement frequencies which substantially override the gains from the reduced displacement frequencies. These systems are disclosed in “An Introduction to Band-Pass Loudspeaker Systems” by Earl R. Geddes, in the Journal of the Audio Engineering Society, May 1989 issue.

Additional loudspeaker enclosure designs have been introduced to attempt to create smaller low frequency systems that can reproduce lower frequencies and play them louder without distortion, such as U.S. Pat. No. 4,628,528, “PRESSURE WAVE TRANSDUCING” by Amar Bose and U.S. Pat. No. 5,092,424 “ELECTROACOUSTICAL TRANSDUCING WITH AT LEAST THREE CASCADED SUBCHAMBERS”, by William Schreiber, et al. These can provide reduced diaphragm motion at a few narrow frequency ranges, but have other portions of the bass range where the diaphragm motion is significantly greater, and may have even poorer performance than an acoustic suspension system at those high displacement frequencies and cannot support full output bass without overloading except at a few narrow frequencies, and so the maximum level capability of the systems over the full range of low frequencies is substantially limited to the output capability of the highest displacement frequency ranges and the reduced displacements in the narrow ranges cannot fully contribute to maximizing undistorted bass output through the bass frequency range.

Other systems have developed variations on these themes, primarily introducing more efficient processing algorithms and refinements, but none that change the fundamental limitations of these approaches to provide large bass system performance in a small device without significantly compromising perceived sound quality and quantity.

There is a still an unfulfilled need for an approach that can improve the perceived bass quantity and extension for a given size of low frequency system, without significantly compromising the bass quality and fidelity.

It would be desirable to have a low frequency loudspeaker enclosure and signal processing system that can maximize the low frequency capability and increase the sound quantity in the low frequency range for a given size enclosure while substantially maintaining the perception of sound quality, providing perceived tonal accuracy and realistic physical bass impact.

Applicant hereby incorporates herein by reference any U.S. patents and U.S. patent applications, and technical papers cited or referred to in this application to the extent the prior disclosure is consistent herewith, and to the extent inconsistent, this later disclosure shall control.

SUMMARY

A loudspeaker system with a signal processor for enhancing low frequency output capability provides a system that can minimize loudspeaker overload distortion at high level, low frequency, audio signals, while maintaining perceived tonal quality and physical bass impact quantity. One example of the loudspeaker system and signal processor comprises a loudspeaker enclosure system, including at least one low frequency transducer with a vibratile diaphragm, wherein the enclosure system includes at least one resonant chamber, the resonant chamber comprised of a bass-reflex resonant chamber or a wave-resonant air column chamber, including at least one resonant chamber resonance tuning frequency (F_(RC1)) creating a first frequency range of reduced diaphragm displacement with the tuning frequency at which the displacement characteristic of the vibratile diaphragm as a function of frequency has a minimum. The enclosure system also has a second frequency range, adjacent to, and above the first frequency range, in which there is a frequency at which the displacement characteristic, as a function of frequency above the resonant chamber resonance frequency F_(RC1), has a maximum (F_(MAX1)). The loudspeaker system further includes a multi-modal signal processor. At small signal levels a starting, target frequency response may be established, either by loudspeaker enclosure/transducer parameters and/or filter gain equalization. A threshold detector for detecting a primary amplitude threshold is established in the signal processor for sensing an audio signal amplitude threshold in the second frequency range. When the audio input signal exceeds the primary amplitude threshold, a gain filter mode, incorporating a dynamic narrowband filter, reduces the gain in the second frequency range, a harmonics controller, incorporating a dynamic harmonics generator to dynamically generate harmonics in a third frequency range, above F_(MAX1), and the third frequency range exhibiting a reduced diaphragm displacement as compared to frequency F_(MAX1).

The harmonics produced by the dynamic harmonics generator create a virtual fundamental tonal gain in the second frequency range that corresponds to gain reduced fundamental frequencies in the second frequency range to create at least a partial tonal gain replacement for the gain reduced frequencies in the second frequency range. When operating above the threshold, the gain in the first frequency range is preferably maintained above that of the gain in the second frequency range, maintaining the real and perceived lower frequency physical impact. When operating at small signal levels, below the primary threshold level, the activity of the dynamic narrowband filter in the second frequency range is inactive. When operating at small signal levels, below the primary threshold level, corresponding activity of the dynamic harmonics generator may also remain inactive.

When the primary narrowband audio amplitude threshold is exceeded, the primary dynamic narrowband filter is activated and the dynamic harmonics generator is cooperatively activated with the dynamic narrowband filter, and as a level of an audio input signal within the second frequency range is increased further, the gain of the primary dynamic narrowband filter is reduced and the harmonics gain of the dynamic harmonics generator is increased.

When operating above the primary narrowband amplitude threshold the signal processor operates with the dynamic narrowband filter gain and the dynamic harmonics generator gain correspond in an inverse relationship to each other, and as the filter gain in the second frequency band is dynamically reduced to minimize an audible overload distortion, a first frequency range acoustic level is substantially maintained relative to that of an acoustic level of the second frequency range, to more effectively maintain a perceived physical bass impact, and the harmonics gain in the third frequency range is increased to more effectively maintain a perception of a tonal level in the second frequency range.

The dynamically gain reduced frequencies in the second, displacement sensitive frequency range and the tonal replacement of those frequencies by the dynamic harmonics generator, when used in this manner so aligned with an enclosure with the resonant chamber, allows the system to operate at significantly greater output levels without low frequency overload, while substantially maintaining the perception of tonal and physical impact fidelity.

In another example of the loudspeaker system with multimode signal processor, the system as described above is further enhanced with inclusion in the signal processor of a transpositional gain controller, incorporating a dynamic transpositional gain controller, whereby when the threshold is exceeded and the dynamic narrowband filter reduces gain the second frequency range, frequencies in the second frequency range may be transposed as additional gain to a frequency in the first, displacement reduced, frequency range, preferably at or near the resonant chamber resonance frequency in the first frequency range, to in a manner corresponding to the gain reduction of the gain reduced frequencies in the second frequency range, further replace or maintain any loss in physical impact caused by the reduction in output from gain reduced frequencies in the second frequency range. The gain of the frequencies transposed by the transpositional gain controller may be balanced in level with the gain the harmonics generated in the third frequency range, such that the generated harmonic and the generated transpositional gain together replace the reduced gain in the second frequency range with optimal tonal fidelity and physical impact fidelity. This multi-modal approach used in this manner in conjunction with a resonant mode, enclosure architecture with an resonant chamber resonance frequency allows the tonal and physical impact replacement of gain-reduced frequencies in the second frequency range to maintain the loudspeaker system fidelity to increased output levels while maintaining fidelity and avoiding overload distortion in a manner emulating a larger, higher output loudspeaker system.

By having the multi-modal processes of the signal processor being dynamic, such that in some examples of the loudspeaker system with a signal processor for enhancing low frequency output capability, they may remain inactive at small signal levels, and may be activated at large signal levels, the system maintains high fidelity at small or average signal levels without any dynamic processing, and operating with the target frequency response without overload distortion.

As a further example loudspeaker system, supplementing either of the examples of the loudspeaker system disclosed above, in a fourth frequency range, below the resonant chamber resonance frequency of the first frequency range, a first additional gain filter may be employed with the additional filter being at least one of a high-pass filter and a narrowband filter, and the filter may also be one of a fixed gain filter and a dynamic gain filter, wherein when the first additional filter is operated as a dynamic gain filter, it is activated by a secondary amplitude threshold detected within the fourth frequency range. Upon the threshold being exceeded and the gain being reduced dynamically in the fourth frequency range, one or both of the transpositional controller and the harmonics generator may be activated to transpose the reduced gain from the gain reduced frequencies in the fourth frequency range to a dynamic gain in the first frequency range, at or near the resonant chamber resonance frequency in the first frequency range, and the harmonic generator generates harmonics of gain reduced fundamental frequencies in the fourth frequency range. These and other attributes will be come apparent as examples of the loudspeaker system with signal processing are further described herein.

BRIEF DESCRIPTION OF THE DRAWINGS

The figures depict examples of the present invention for the purposes of illustration only. One skilled in the art will readily recognize from the following discussion that alternative embodiments of the structure and methods illustrated herein may be employed without departing from principles described.

FIG. 1 is a first example loudspeaker system bass-reflex resonant chamber loudspeaker enclosure with a passive acoustic port radiator and low frequency signal processor;

FIG. 2 is a spectral representation of one example of native amplitude response, target small signal amplitude response, and impedance curve;

FIG. 3 is a graphic representation of the diaphragm displacement as a function of frequency of the bass-reflex resonant chamber loudspeaker enclosure of FIG. 1;

FIG. 4 is spectral representation of the dynamic harmonics generator;

FIG. 5 is another example graphic representation of the diaphragm displacement as a function of frequency;

FIG. 5A is graphic representation of the operation of dynamic narrow band gain filters;

FIG. 6 is another example of the loudspeaker system and signal processor further including a dynamic transpositional gain controller;

FIG. 7 is a graphic representation of the diaphragm displacement as a function of frequency of a resonant chamber loudspeaker and the dynamic transpositional gain controller;

FIG. 8A is a graphic representation of the dynamic filter gain, dynamic harmonics gain, and dynamic transposed frequency gain below and above the threshold;

FIG. 8B is a graphic representation of displacement limited acoustic output with an example of the invention and without;

FIG. 8C is an additional example graphic representation of the dynamic filter gain, dynamic harmonics gain and a dynamic transposed frequency gain below and above threshold;

FIG. 9 is a bandpass resonant chamber loudspeaker enclosure including a bass-reflex resonant chamber and a sealed acoustic suspension chamber;

FIG. 9A is a bandpass resonant chamber loudspeaker enclosure including a bass-reflex resonant chamber and a sealed acoustic suspension chamber with an extended vent;

FIG. 9B is a dual tuned bandpass resonant chamber loudspeaker enclosure including two bass-reflex resonant chambers and a sealed acoustic suspension chamber;

FIG. 10 is another dual tuned bandpass resonant chamber loudspeaker enclosure including two bass-reflex resonant chambers;

FIG. 10A is a triple tuned bandpass resonant chamber loudspeaker enclosure with three bass-reflex resonant chambers;

FIG. 11 is a multi-resonant chamber loudspeaker enclosure including a wave-resonant air-column chamber;

FIG. 11A is a resonant chamber loudspeaker enclosure including a bass-reflex resonant chamber coupled to a wave-resonant air-column chamber;

FIG. 12 is a multi-resonant regenerative wave-resonant air-column chamber loudspeaker enclosure;

FIG. 13 is a multi-resonant dual flare wave-resonant air-column chamber loudspeaker enclosure;

FIG. 14A is a graphic representation of impedance magnitude as a function of frequency of a multi-resonant, multi-tuned resonant chamber loudspeaker enclosure;

FIG. 14B is a graphic representation of the diaphragm displacement as a function of frequency of a multi-resonant, multi-tuned resonant chamber loudspeaker enclosure;

FIG. 15 is another example bass-reflex resonant chamber loudspeaker enclosure and signal processor;

FIG. 15A is a graphic representation of the diaphragm displacement as a function of frequency of the resonant chamber loudspeaker and the dynamic transpositional gain controller of FIG. 15;

FIG. 16 is still another example bass-reflex resonant chamber loudspeaker enclosure and signal processor;

FIG. 16A is a graphic representation of the amplitude and gain level as a function of frequency of the resonant chamber loudspeaker system and signal processor of FIG. 16;

FIG. 17 is an example signal processor system;

FIG. 18 is an example subwoofer enclosure system with bass-reflex resonant chamber and a sealed, acoustic suspension chamber and corresponding signal processor;

FIG. 19 is an example subwoofer enclosure and a smaller upper range loudspeaker enclosure system and signal processor;

FIG. 20 is graphic representation of the diaphragm displacement of a subwoofer enclosure and a smaller upper range loudspeaker enclosure system and signal processor of FIG. 19;

FIG. 21 is graphic representation of the dynamic harmonics generation of a bandpass subwoofer enclosure when used with a smaller upper range loudspeaker enclosure system and signal processor of FIG. 19;

FIG. 22 is graphic representation of the dynamic harmonics generation of a smaller upper range loudspeaker when used with a bandpass subwoofer enclosure system and signal processor of FIG. 19;

FIG. 23 is another example of the loudspeaker system with bass-reflex resonant chamber loudspeaker enclosure and a real-time example of the signal processor.

FIG. 24 is graphic representation of one set of gain filter contours for a narrowband gain filter, a high-pass gain filter and a shelf gain filter.

FIG. 25 is another example of the loudspeaker system and signal processor showing interactive modal processing blocks and a low frequency enclosure with a bass-reflex resonant chamber and a sealed, acoustic suspension chamber.

DETAILED DESCRIPTION

FIG. 1 represents a first example 10 a of the inventive loudspeaker system, including a multi-mode signal processor 22 for minimizing audible overload distortion while increasing perceived low frequency output capability, comprising at least one loudspeaker enclosure 12, including at least one low frequency resonant chamber 16 and at least one electro-acoustical transducer 18, with a vibratile diaphragm 64 for converting an input electrical signal, which may be an input audio electrical signal, received at input 23, and amplified by amplifier 20 to amplifier output/loudspeaker input point 21 a, into a corresponding amplified acoustic output signal 26, including a resonant chamber output 26 a, with the resonant chamber 16 consisting of at least one of a bass-reflex resonant chamber and a wave-resonant air-column chamber, with the example loudspeaker system of FIG. 1 showing a bass reflex enclosure 12 with resonant chamber 16. The acoustic mass of the passive acoustic radiator 14 a, and the compliance of the air volume in chamber 16 form a bass-reflex resonance creating the resonant chamber resonance tuning frequency (F_(RC1)) 34 in graph 30 a of FIG. 3. Passive acoustic mass radiator 14 a, us shown in FIG. 1 as an open vent or port, but may optionally be interchanged with a passive diaphragm radiator, as shown in FIG. 6 as 14 b.

Also referring to FIG. 3, the loudspeaker system 10 a includes a first frequency range 32 with a reduced diaphragm displacement and a fundamental resonant chamber resonance frequency 34 at which a displacement characteristic of the vibratile diaphragm 64 as a function of frequency has a minimum 34 a.

The loudspeaker system 10 a also includes a second frequency range 36, adjacent to, and higher in frequency than, the first frequency range 32, includes an increased diaphragm displacement and a frequency (F_(MAX1)) 37 a, at which the displacement characteristic of the vibratile diaphragm 64 as a function of frequency has a maximum 37 a. The system also includes a third frequency range 39, above the frequency F_(MAX1) 37 a.

Additionally, the system 10 a includes multi-mode signal processing block 22, with a primary dynamic narrowband filter 25 for primarily dynamically adjusting a gain of one or more frequencies within the second frequency range 36, and a processing block 22 with a harmonics controller, configured to include a primary dynamic harmonics generator 27 to produce harmonics 74 (shown in FIG. 4) in the third frequency range 39 and dynamically adjusting a harmonics gain in the third frequency range 39 with the produced harmonics 74 corresponding to the dynamically gain adjusted frequencies 36 b within the second frequency range 36 and the produced harmonics 74 creating a virtual frequency gain replacement 72 for gain adjusted frequencies 36 b in the second frequency range 36. Frequency range 39 may extend upward in frequency as far as needed to for the selections of produced harmonics to create the most effective virtual fundamental frequency gain in a gain reduced frequency range.

Referring to FIG. 1, and also FIG. 8A, a threshold detector and activator 24 is configured to detect a primary narrowband audio amplitude 120 threshold 122 (of FIG. 8A) based on an audio drive signal at amplifier 20 output 21 a corresponding to a displacement of the transducer 18 diaphragm 64 within the second frequency range 36, and, the displacement threshold 122 may correspond to an audible overload distortion of the transducer 18 acoustic output 26.

In an example loudspeaker system and signal processor, when a corresponding amplified audio signal level 120 is below the primary narrowband amplitude threshold 122, the primary dynamic narrowband filter 25 and the primary dynamic harmonics generator 27 is inactive. When the primary narrowband audio amplitude threshold 122 is exceeded, the primary dynamic narrowband filter 25 is activated and the dynamic harmonics generator is activated 27, and as a level of an audio input signal within the second frequency range is increased further 124, the dynamic filter gain 125 of the primary dynamic narrowband filter 25 is reduced further preferably holding the displacement of diaphragm 64 to a maximum limited amplitude to minimize overload distortion, and the dynamic harmonics gain 126 of the dynamic harmonics generator 27 is increased, such that when operating at amplitude levels 120 above the audio amplitude threshold 122 the signal processor 22 operates with the dynamic narrowband filter 25 gain 125 and the dynamic harmonic generator 27 gain 126 corresponding in an inverse relationship to each other wherein as the dynamic filter gain 125 in the second frequency band 36 is dynamically reduced to minimize audible overload distortion, the first frequency range 32 acoustic level is substantially maintained relative to that of the acoustic level of the second frequency range 36, to more effectively maintain a perceived physical bass impact, and the dynamic harmonics gain 126 in the third frequency range 39 is increased to more effectively maintain a perception of a tonal level 72 (FIG. 4) in the second frequency range 36.

The threshold detector/activator 24 may be optimized with a predictive model to predict threshold parameters for loudspeaker system 10 a, including transducer 18, and compare to an analysis of the input signal directly or the corresponding amplified audio signal after a volume/gain control setting of an amplifier 20, which may include predictive information about the forward gain profile of the amplification circuits to the point of the output 21 a of the amplifier 20. Alternatively, the system may sense a signal level, or distortion level, and use feedback 21 to the threshold detector/activator block 24 from a point from the output 21 a of amplifier 20 (which may be equivalent to loudspeaker 12 or transducer 18 input). Also feedback 21 may be derived from a sensor 49 at the loudspeaker transducer 18 output, sensing acoustic output 26, or diaphragm 64, displacement. The sensor may be coupled to the diaphragm 64 of transducer 18 or may be mounted on the transducer or suspended near the transducer diaphragm 64. The primary threshold may be a diaphragm 64 displacement limit relative to approaching the onset of a predetermined acoustic level or audible distortion level. A threshold may also relate to a transducer voice coil temperature reaching a level of either raising the impedance of the transducer to create an onset of distortion/compression, or voice coil temperature relative to overheating or potential damage. The threshold may also relate to an amplifier 20 overload level, or clipping, as the level approaches, or exceeds, a predetermined level or audible distortion level. The threshold detector 24 may have one or more thresholds to trigger the activation processing modes of the signal processor 22, and some of which may be secondary thresholds that may relate to additional parameters of the loudspeaker system and may activate different aspects of the processor or control one or more frequency ranges of the loudspeaker system.

The control structures of the first example 10 a of the loudspeaker system and signal processor incorporate separate dynamic narrowband filter 25 and dynamic harmonics generator 27 processes and may utilize an asymmetrical attack and release time with substantially instantaneous dynamic gain filter reduction onset, and slower, or longer gain recovery time, preferably at least 4 times longer than the attack time, to minimize audible distortion artifacts, or audible pumping distortion, from the dynamic narrowband filter 25 and to optimize control of the harmonics of the dynamic harmonic generator 27 independently of the dynamic narrowband filter 25 for optimization of harmonic levels, and generation and control of an all even harmonics only, all odd harmonics only, or a controlled mix of even and odd harmonics. Additionally, the harmonics generator may include a harmonics shaper to vary the gain level of one or more harmonics relative to the other harmonics, such as shaping the harmonics such that each higher harmonic number may be attenuated relative to each lower adjacent harmonic number, i.e. as seen in FIG. 4, showing generated harmonics 74, with a second harmonic 74 a, followed by a reduced level, third harmonic 74 b, followed by a further reduced level, fourth harmonic 74 c, and 74 d representing any additional harmonics, of which one or all may be lower in level than all preceding harmonics. In any of the example systems the harmonics 74 may be represented by as few as two harmonics or by an extended series of harmonics, of three or greater.

As the dynamic narrowband filter, operates as a narrowband gain controller in second frequency range 36, it may preferably allow the frequencies below (and above) narrow threshold band 36 (of FIG. 2) to remain substantially unaffected, by the primary function of dynamic narrowband filter 25, supporting the resonant chamber resonance frequency 34 in the first frequency range 32 and the frequencies in the third frequency range 39 operating substantially without gain attenuation, unless enacted by predetermined additional process control in signal processor 22.

An organization of the control blocks within signal processor 22 are such that the threshold detector/activator 24 is in series with and ahead of following processor blocks of, the dynamic narrowband filter 25 and dynamic harmonic controller/generator 27, which operate in parallel with each other and couple the output to amplifier 20 in this example system. The threshold detector/activator 24, upon reaching a predetermined threshold, can active the dynamic narrowband filter 25, and the dynamic harmonics controller/generator 27, substantially simultaneously.

Alternatively, in other example systems, all the gain blocks in signal processor 22 could operate in series, for instance, the threshold detector/activator 24 could activate dynamic narrowband filter 25, which could serially activate the dynamic harmonics controller/generator 27 upon a gain reduction being activated in the dynamic narrowband filter.

FIG. 2 includes a spectral graph representation 30 of an example of a passive, pre-processed, native system amplitude response 35 a and one example of a reference, or target small signal response 35 b representing a frequency response of a system operating below the amplitude threshold. When reducing the size of a given loudspeaker system, or optimizing a system to be more efficient, the response in the lower frequency range may droop, or attenuate in amplitude as a function of a reduction in frequency, as shown in the native response curve 35 a. In one example system of the loudspeaker system with signal processor, the amplitude may fall in response at a rate per octave through first range 32 and second frequency range 36, operate substantially flat over the third frequency range 39, and fall at a steeper slope in the fourth range 40, below the first frequency range 32. This reduction in low frequency response may allow for an overall loudspeaker system design that provides greater system efficiency in, and in some enclosure types, above the third frequency range 39. This native response with low frequency attenuation may allow the enclosure size to be reduced for a given efficiency above the second frequency range 36. The upper high-pass corner frequency is shown at the intersection frequency range 36 and frequency range 39, but system parameters may also be chosen to have the transition be somewhat above or below this frequency intersection frequency. In some system alignments, the native response 35 a may be a preferred starting, passive frequency response of transducer 18 and enclosure 12 before applying any electronics or equalization. The reference target curve may have a preferred response that is a substantially flat frequency response to as low a frequency as possible, plus or minus an amplitude tolerance error but may have a somewhat different amplitude response, that achieves a preferred tonal balance, or match to an environment, or use model. The reference target curve may be achieved with transducer 18 and enclosure 12 parameters, or may be a fixed, starting electronic equalization applied to the native passive response to achieve a preferred reference target small signal curve. As an example 10 a in FIG. 1 the system may be equalized to have a substantially flat, starting frequency response, with the term “starting frequency response” referring to a small signal response, when operating below the amplitude threshold, before the dynamic narrowband filter is activated upon the amplitude threshold being exceeded, wherein the amplitude threshold relates to the narrow band second frequency range. The term narrowband, in the dynamic narrowband filter 25 and the bandwidth of the second frequency range 36, may refer to a bandwidth of approximately two octaves or less, and, in some examples, may be less than one octave, to maintain more bandwidth of non-gain reduced frequencies at and above the first frequency range, while still avoiding the perception of audible overload distortion, by dynamically suppressing gain in the high excursion frequency range 36, and particularly frequencies near a maximum excursion frequency such as F_(MAX1) 37 b, as shown in graph 30 a of FIG. 3. The signal processing block 22, with dynamic narrowband filter 25 and dynamic harmonics generator 27, is deployed to maintain aural and physical impact perception fidelity to a preferred target response curve, such as example target curve 35 b while minimizing audible overload distortion of loudspeaker system 10 a.

Also shown in FIG. 2 is enclosure/transducer impedance curve 31, corresponding to the example shown in FIG. 1, wherein an impedance minimum 31 b corresponds to resonant chamber resonance frequency F_(RC1) 34 in first frequency range 32. Transducer resonance impedance peak 31 a may be within frequency range 40 or at the lower frequency portion of frequency range 32, and transducer impedance peak 31 c may fall within second frequency range 36 or may be at a somewhat higher frequency, in frequency range 39.

The frequency of the resonant chamber resonance F_(RC1) 34 can be seen as corresponding to an impedance minimum as a function of frequency, and represents the resonant chamber resonance, with the frequency 34 defined primarily by the enclosure volume 16 compliance and passive acoustic radiator acoustic mass, substantially independent of the transducer parameters, whereas the frequencies of impedance peaks 31 a and 31 c are transducer resonances determined by the combination of transducer Thiele-Small parameters and the enclosure parameters.

Resonant chamber based loudspeakers of the loudspeaker system and signal processor, including resonant bass-reflex and resonant air-columns, exhibit at least one chamber resonance causing the loudspeaker system 10 to exhibit a fundamental resonant chamber resonance frequency 34 at a low operating frequency range where the diaphragm displacement as a function of frequency is minimized as opposed to a, non-resonant chamber based enclosure, such as an acoustic suspension or open baffle for which there is no resonant chamber resonance or diaphragm displacement minimum as a function of frequency, and transducer diaphragm motion is increased at low frequencies.

Referring again to FIG. 3, showing diaphragm displacement graph 30 a, wherein the vertical portion of the graph represents diaphragm displacement for a given constant driver voltage and the horizontal portion of the graph represents frequency. Frequency range 32 is a reduced diaphragm displacement range, including fundamental resonant chamber resonance frequency F_(RC1) 34 with transducer 18 diaphragm 64 displacement minimum 34 a, which as a function of frequency represents a significant reduction in diaphragm excursion relative to adjacent frequencies for a constant input voltage vs. frequency to the transducer 18 in enclosure 12 of FIG. 1. The second frequency range 36 is an increased diaphragm displacement range, with a maximum displacement frequency 37 a which can be a primary limiting factor relative to displacement limited output capability of the loudspeaker system 10 a. A woofer transducer will have a diaphragm displacement limit wherein various components in the transducer, such as the suspension and magnetic circuit with voice coil, have been required, by the audio signal program material, to move so far as to have its movement become non-linear, which may result in audible overload distortion. Upon the audio input signal containing frequencies in frequency range 36 that increase in amplitude to the level that a diaphragm 64 displacement threshold is exceeded, the threshold detector 24 may activate the dynamic narrowband filter to start attenuating frequency range 36 in a manner shown in narrowband gain reduced curve 36 b. By gain reducing frequency range 36 with a narrowband filter, frequencies above and below frequency range 36 may remain substantially unaltered, and the loudspeaker system can play louder overall without audible overload distortion. Below frequency range 32 is a fourth frequency range 40 which is another higher displacement frequency range with frequency 37 b representing a displacement maximum, which may be a peak, or a maximum reached that continues at the same level substantially down to below 1 Hz. The diaphragm displacement in frequency range 40 is much greater than frequency range 32 for the same voltage input to the transducer 18. In this range a fixed filter may be incorporated into equalization built into signal processor 22, such as a high-pass filter or a narrowband filter, with a gain reduction curve like the one shown as high pass filter curve 40 b or narrowband filter 40 c. Fixed, in this case meaning that the gain of the curve as a function of frequency is constant with input voltage level. In some embodiments of the loudspeaker system and signal processor this may be a dynamic high pass filter, with a non-linear gain relative to input voltage. Curve 40 a represents the diaphragm displacement for the loudspeaker in FIG. 1, without the high pass filter. The implementation of high pass filter curve 40 b or narrowband filter 40 c may allow the system to substantially increase total output without being overloaded in frequency range 40 by low frequency, or subsonic frequencies which may overload the transducer 18 diaphragm 64 displacement capability, causing audible overload distortion, and potential damage to the transducer 18. This high-pass filter may be of any order, but preferably it is at least a second, or higher, order high pass filter to effectively reduce gain adequately to avoid diaphragm overload under worst case program material conditions with very high level, low frequency audio, or subsonic signals. The filter may also be an under-damped high-pass filter as part of establishing the reference target frequency response, by having the under-damped characteristic cause a gain boost in frequency range 32 and in some embodiments, at least a portion of the frequency range 36, while applying significant attenuation to a significant portion of frequency range 40. While “Q” values for an under-damped filter may be of any useful value to compliment the particular system parameters, but generally a range between a “Q” of 1.4, with 3 dB of peaking, and a “Q” of 4, with 12 dB of peaking, would be preferred.

Any of the examples of the loudspeaker system and signal processor may additionally have a starting, fixed equalization, to a predetermined, target small signal response shape, as a starting spectral balance and frequency response curve.

FIG. 4 shows dynamic gain and harmonics generation in amplitude/gain level graph 30 b showing frequency range 36 and frequency range 36 being represented with significant gain reduced frequency curve example 36 b. Frequency 34 shows chamber fundamental, resonant chamber resonance tuning frequency F_(RC1) as being maintained at a substantially full gain level during an overload protective gain reduction being applied to frequency range 36 as discussed above. When frequency range 36 is gain reduced, to minimize diaphragm 64 displacement, the harmonics generator produces harmonic series 74 in frequency range 39, including harmonics, 74 a, 74 b, 74 c, (74 d representing more or less included harmonics as they may be even or odd harmonics or a mix of both and may be carried up to a higher harmonic count or limited to just the lower harmonics first, second, third, and may be attenuated with each increasing harmonic number) creating perceived, virtual fundamental frequency 72 at reference target level 36 a as the harmonics create a psycho-acoustic, virtual pitch representation of the suppressed fundamental frequencies 36 b which is perceived by the listener as substantially the same tonal character and tonal level 36 a as that frequency range before it was gain reduced to curve 36 b and it is perceived at substantially full gain level 36 a, creating a virtual fundamental 72, tonally duplicating the fundamental as if it had not been gain reduced. This can be applied to one or more gain reduced fundamentals in the frequency range 36.

This balance of having the gain reduced in frequency range 36 to protect from audible overload distortion, and the harmonics in frequency range 39 having a corresponding gain increase to create virtual tone replacement frequencies 72 maintains the perceived tonal balance of the loudspeaker system while allowing the system to operate at much greater output levels while minimizing audible overload distortion. Also, by maintaining the system gain at frequencies in frequency range 32, much of the perceived physical impact from reproduced bass frequencies is preserved such that the system minimizes overload distortion while playing louder, while sustaining tonal and physical impact fidelity. Frequency range 40 for this example shows a high pass filter characteristic similar to that shown in FIG. 3 and described above.

In an example loudspeaker system with signal processor, the dynamic harmonics generator 27 can operate effectively for a given gain suppressed frequency band of two octaves or less, and in some examples when creating a virtual tonal replacement of approximately 1.5 octaves or less, and the bandwidth of the dynamic narrowband filter has a maximum bandwidth of less than two octaves, and in some examples of the loudspeaker system, approximately 1.5 octaves or less, and to have the narrowband gain filter bandwidth 36 b and the harmonics generator virtual fundamentals 72, within frequency range 36, have a bandwidth that substantially matches the gain reduced bandwidth 36 b. Beside the bandwidths corresponding between the narrowband filter and the virtual tones of the harmonics generator, the gain reduction of the narrowband filter and the gain increase of the generated harmonic series 74, should have a corresponding inverse gain relationship to have the tonal effect of the narrowband gain reduction 36 b be at least partially perceptually replaced by the perceived level of the virtual tone or tones, 72. It is advantageous to have the perceived level of the virtual tone or tones, 72 create a perception of the same tonal quality as if the gain reduced frequencies had not been gain reduced.

FIG. 5 shows a graph 30 c displaying ‘diaphragm displacement’ (or excursion) in the vertical, and frequency in the horizontal, similar to that shown in FIG. 3, wherein a first frequency range 32 with reduced diaphragm displacement, including fundamental resonant chamber resonance frequency 34, also referred to herein as F_(RC1), corresponding to diaphragm displacement minimum 34 a as a function of frequency, which is caused by the fundamental resonance frequency 34 of a resonant chamber in a loudspeaker enclosure, the resonant chamber being one of a bass reflex (or Helmholtz-reflex) chamber, or a wave-resonant air-column chamber, where in this example, referring to loudspeaker system in FIG. 1, the resonant chamber is that of a bass reflex chamber 16 with a resonance frequency 34.

Also shown is a second frequency range 36 with an increased diaphragm displacement, including a maximum displacement frequency 37 a, the second frequency range adjacent to, and higher in frequency, than the first frequency range 32, and the second frequency range including a maximum displacement frequency 37 a, also referred to herein as F_(MAX1). The frequency range 36 is also represented with small signal, below amplitude threshold, full gain response 36 a, and dynamic gain reduced response, as an example curve illustration 36 b when dynamic narrowband filter 25 (FIG. 1) is activated. This curve differs from that of FIG. 3 by way of additional filter curve choices 40 d and 40 e, in the fourth frequency range 40 which adjacent and below first frequency range 32, with maximum displacement frequencies 37 b, full gain response show as curve 40 a, having an optional dynamic gain reduced response, as two examples shown in 40 d or 40 e with one of a dynamic high-pass filter shape example 40 d and a dynamic narrowband filter shape example 40 e with this dynamic filter. This illustration of dynamic filter responses can be used with any of the enclosure systems disclosed herein, but can have particular value when used with the resonant chamber, bandpass enclosures of FIG. 9, FIG. 9A and FIG. 9B, with at least one resonant chamber 16 and sealed chamber 13.

Referring to the loudspeaker system 10 a with signal processor 22, in FIG. 1, the dynamic narrowband filter block may include secondary band-limited dynamic filters, to perform the dynamic high-pass curve 40 d or dynamic narrowband curve 40 e gain reductions upon reaching a secondary band-limited threshold, embodied in the threshold detector/activator 24. The secondary band limited threshold would be coordinated with monitoring or predicting a signal amplitude in frequency range 40, such that upon reaching a predetermined secondary threshold, a gain adjustment process, would be invoked to include a dynamic gain reduction curve 40 d or 40 e. As with the primary threshold detection and primary dynamic gain reduction in frequency range 36, the dynamic gain reductions in frequency range 40 would be dormant when below the secondary band-limited threshold level, and active when at or above the secondary band-limited threshold level. Also, as with the dynamic filter operation in frequency range 36, the band limited dynamic filter operation in frequency range 40 would leave frequency range substantially unaffected by the gain reduction in frequency range 40.

Additionally, a secondary harmonics generator may operate in coordination with the secondary dynamic gain reduction filter such that as the gain is reduced in frequency range 40, a virtual tone gain is activated and increased in frequency range 40 by way of corresponding harmonics and corresponding harmonics gain being generated in a frequency range above frequency range 40 to sustain a perception of a pre-gain-reduced tonal level and fidelity of frequency range 40.

The harmonics generated in correspondence with gain reduced frequencies in frequency range 40 may fall within frequency range 39 a, which may extend below frequency range 39 to a frequency within frequency range 32. As program material, such as music or movie soundtracks, changes dynamically on a moment to moment basis when high intensity input signals are in the range of frequency range 40, the program material may be lessened in frequency range 36, such that at least a portion of frequency range 36 may be available for generated harmonics supporting gain reduced frequencies in frequency range 40. Some portion of frequency range 39 or 39 a may support generated harmonics for frequency range 40. It may be the case that if frequency range 36 was being gain reduced to avoid audible overload that additional generated harmonics gain may or may not be produced in the portion of frequency range 39 a that overlaps with frequency range 36.

FIG. 5A represents one example of dynamic filter gain curves vs. frequency graph 30 d illustrating the primary dynamic narrowband filter 25 gain characteristic 52 of frequency band 36 and one possible secondary dynamic band limited filter gain characteristic 62 optional band-limited, secondary dynamic gain filter of frequency band 40. The system resonant chamber enclosure's fundamental resonant frequency (F_(RC1)) is shown at 34 residing within the first frequency range 32. Small signal, reference target small signal gain/amplitude response curve 51 shows the relative preferred frequency response curve upon the dynamic systems being in a substantially dormant state below the predetermined threshold levels. Upon the second frequency band 36 having an amplitude within a signal frequency that drives the transducer diaphragm to a displacement amplitude threshold in frequency band 36, a gain within frequency band 36 is gain reduced by the amount required to maintain the diaphragm displacement in that band from exceeding the predetermined overload threshold. The multiplicity of gain reduced curves 52 show a progression of greater and greater activity of gain reduction of the dynamic narrowband filter, with increasing audio signal level, from no gain reduction 52 a when below threshold, to gradually increasing gain reductions 52 b thru 52 e such that approximately equal excursion is reached over a useful range of levels, the excursion set by the maximum limits prior to audible overload of the loudspeaker transducer diaphragm 64 displacement.

During all these gain reductions it can be seen that frequency F_(RC1) 34 remains substantially at full gain, maintaining a perceived physical bass impact.

Optionally, as a additional performance enhancement and avoidance of overload, a fourth frequency range 40 may also have a dynamic gain reduction filter applied upon the threshold detector 24 applying a second threshold set to the frequency range 40 starting below the threshold with non-gain reduced curve 62 a and the progressively increased gain reduction of curves 62 b thru 62 e.

As in the embodiments described above, as the threshold is exceeded and the gain is reduced in the second frequency range 36 the perceived tonal gain in the band 36 will be substantially replaced and maintained by the activation of the dynamic harmonics generator adding harmonics that are harmonics of gain reduced fundamental frequencies within band 36 with appropriately increased gain to create and maintain a perception of a maintained tonal balance of the gain reduced fundamentals in range 36, by way of virtual fundamental frequencies replacing reduced gain frequencies in range 36, which would be lost without the support of the dynamic harmonics in frequency range 39. The harmonics of frequencies within frequency band 36 will be created predominately above frequency band 36 where full gain will tend to be available without driving the transducer to audible overload, as frequency band 36 will tend to operate with a bandwidth of less than two-octaves, and in most embodiments, less than 1.4 octaves, and in one preferred embodiment, with approximately 1.25 octaves of bandwidth or a frequency multiplier of 2.5.

The optionally gain reduced fundamental frequencies in band 40 can also have associated harmonics generated by the dynamic harmonics generator, some of which may fall into the frequency band 36 and some above frequency band 36. As most peak program material varies in frequency and level on a moment by moment basis, it may be that the when either frequency range 36 or 40 are above the specific threshold for their frequency range and therefore gain reduced by the dynamic gain filter, the other frequency range may be below threshold, or at least have less gain reduction at the same point in time, and therefore be available for supporting harmonics generation in that range.

Related to another aspect of the loudspeaker system and signal processor, the inventor has found that for fundamental frequencies below approximately 100 Hz, if the harmonics of those fundamental frequencies are maintained, one can move the fundamental of a tone to another, nearby, frequency without substantially changing the perceived pitch. From this it was found that in the inventive loudspeaker system can benefit from moving, or transposing, at least part of the gain of a fundamental frequency of a rich harmonic tone, from a frequency range of greater diaphragm displacement to a frequency of reduced diaphragm displacement, which allows the system to maintain or increase the perceived physical bass impact when reducing the gain of a displacement vulnerable frequency range to avoid audible overload, which also allows the system to play louder overall, without an apparent loss of physical bass impact. This approach can maintain a convincing perception of fidelity, particularly if the real tones and harmonics are intact at low and average sound levels, or if harmonics are added to enhance the tonal quality when transposing the fundamental frequency to a higher or lower frequency. It may be perceptually convincing to transpose the gain of a fundamental frequency by no more than two octaves and in some examples of the loudspeaker system, by one octave or less.

Also, when transposing a gain of the physical impact fundamentals from a high displacement frequency range, such as frequency range 36, and applying or a corresponding gain to a lower displacement frequency, such as resonant chamber frequency 34, frequency range 36 can be made somewhat wider in bandwidth, to further abate overload distortion at higher levels while effectively replacing a greater amount of physical impact frequencies that are gain reduced, by transposing the frequencies of the second frequency range 36 to a low displacement frequency in the first frequency range 32, preferably the lowest displacement frequency 34 a, the resonant cabinet resonance frequency F_(CR1) 34.

Loudspeaker system 10 b of FIG. 6 shows a second example of the loudspeaker system with low frequency signal processor 22, including resonant chamber enclosure 12 a, woofer transducer 18, including a vibratile diaphragm 64. The loudspeaker system 10 b further includes at least one bass-reflex resonant chamber 16, and passive acoustic mass radiator 14 b, shown here as a passive diaphragm radiator, but can optionally be interchanged with an elongated vent or port, as shown in FIG. 1 as 14 a. The transducer 18 is driven by amplifier 20 and connected to the input of the amplifier 20 is the multi-mode signal processor block 22, including threshold detector/activator 24, a gain filter, incorporating a dynamic narrowband filter 25, a harmonics controller, incorporating a dynamic harmonics controller generator 27, and transpositional gain controller incorporating a dynamic transpositional gain controller 29.

Referring to loudspeaker system 10 b in FIG. 6 and graph 30 e of FIG. 7, at small signal levels, the dynamic processes of the processing block 22 will remain substantially dormant until an audio input signal, received by audio input 23, and amplified to output 21 a by amplifier 20, increases to a level where an amplitude threshold is exceeded, upon which the threshold detector/activator 24 activates the dynamic narrowband filter 25 to reduce gain (as shown in curve 36 b) in a second frequency range 36, which is adjacent to, and above, a first frequency range 32, which contains resonant chamber resonance tuning frequency 34. As discussed above, relative to FIG. 1, FIG. 3, FIG. 4, and FIG. 5, upon the activation of dynamic narrowband gain reduction in the designated frequency band 36, as shown in gain reduced curve 36 b, the dynamic harmonics generator 27 creates harmonics in frequency range 39 creating virtual fundamental tones (shown as 72 of FIG. 4) corresponding to the fundamental frequencies being gain reduced in frequency range 36. As the gain in band 36 is reduced from starting displacement level 36 a towards reduced level example curve for illustration, 36 b, the harmonics of frequencies in band 36 b, from an audio input signal, are generated and gain/level set to create a perceived virtual fundamental frequency gain increase in frequency range 36 that corresponds with the gain decrease of fundamental frequencies in frequency range 36, to maintain the same apparent tonal level and balance for frequency range 36 that would be experienced by a listener as having no gain reduction in frequency band 36, as illustrated in FIG. 4 with virtual fundamental 72 being created by the corresponding generated harmonics illustrated as 74 a through 74 d.

Upon the onset of gain reduction in frequency band 36, in addition to the activation of dynamics harmonics controller generator 27, the dynamic transpositional gain controller 29 is also activated wherein frequencies within band 36 that are gain reduced as shown in gain reduction curve 36 b, have at least a portion of the magnitude of their gain reduction, transposed to a frequency at, or near, the diaphragm displacement minimum 34 a resonant chamber frequency 34 within first frequency band 32 with a gain boost example 34 b at the resonant chamber 16 tuning frequency 34 corresponding to the gain reduction 36 b of frequencies in frequency band 36, and the harmonics generator 27 generates harmonics corresponding to the gain reduced fundamentals 36 b. The transposed gain replacement of gain reduced frequencies of frequency 36 is balanced between the tonal gain increase from the dynamic harmonics generator 27, and the physical impact gain increase from transpositional gain controller, such that the perceived balance of tone and physical impact fidelity of frequency range 36 after gain reduction meets a preferred tonal and physical bass impact balance or may be comparable with the perceived fidelity below threshold levels prior to any gain reduction of frequency range 36.

Frequency range 40 may include gain reduction filters creating gain reduced curves 42 b or 42 c reducing gain from the non-gain reduced curve shown as 42 a. The gain reduction filter in frequency range 40 may have a curve shape that is at least one of a high-pass filter and a narrowband filter, and the gain reduction filter for frequency range 40 may also have an activation type to be one of a fixed, or static, gain filter and a dynamic gain filter.

Optionally as a predetermined secondary band limited amplitude threshold is reached for frequencies in frequency range 40 creating as an illustrative example, narrowband gain reduction curve 42 b or high-pass gain reduction curve 42 c, those frequencies and gain corresponding to the amount of reduced gain is dynamically transposed to a frequency of the displacement reduced frequencies in the first frequency range 32, preferably to resonant chamber resonance frequency F_(RC1), 34 with transposed frequency gain illustrated as 34 b. A further option is to have the gain reduced frequencies 42 b utilized as reference frequencies to have the harmonics generator 27 create harmonics creating virtual fundamental tones corresponding to those gain reduced fundamentals 42 b. The harmonics generator may be at least one of a fixed, or static, gain harmonics generator and a dynamic gain harmonics generator. The supplemental process for the gain-reduced frequencies of the fourth frequency range 40 may be one, or both, of the harmonics generator and the transpositional gain controller. The transpositional gain controller may be one of a static transpositional gain controller and a dynamic transitional gain controller. The dynamic or static nature of the transpositional gain controller and harmonics generator may be determined by whether the operational nature of the band limited gain filter in the frequency range 40 is a dynamic or a fixed (or static) gain filter, with it being preferable for the operational aspect of the filter to match that of the harmonics generator and/or transpositional gain controller.

It may be advantageous to utilize the transpositional gain controller of one or more of the loudspeaker system examples to transpose a gain of at least a portion of a diminished amplitude level as a function of frequency that may occur at any of the low frequencies, particularly below 100 Hz, and preferably below 70 Hz, with that gain being transposed to a frequency of reduced diaphragm displacement, to augment a physical impact gain that is lost while minimizing a perception of audible overload of the loudspeaker system, with a tradeoff of overload distortion and perception of physical bass impact being balanced for best overall perceptual performance.

It is perceptually advantageous that the use of transposing the gain of bass frequencies be accompanied by an additional signal process, such as the harmonics generator, to maintain perceptually accurate tonal balance at all signal levels and to override the ear's ability to have the pitch of the transpositional frequency impact the perceived pitch over that of the gain reduced frequencies. It is also a perceptually advantageous feature that the dynamic transpositional gain controller 29 can be dynamic, meaning that it may be dormant and essentially not functional at small signal levels below the amplitude threshold levels. This can be significant with most program material, that most, or all, of the dynamic processes of the signal processing block may be inactive at small signal and/or average level program material, maintaining a low coloration, high fidelity sound quality equivalent to that of a much larger, high quality system without the present loudspeaker system and signal processor, and preferably only activating the multiple signal processing modalities at higher levels, using the interactive modes to maintain, the tonal quality and physical bass impact while being able to increase total system sound pressure levels while effectively minimizing audible overload distortion.

The psychoacoustics of the ear-brain system may establish a large portion of its judgment about a sound based on the sustained average levels, often as much, or even more than the instantaneous peak levels. By maintaining the original, non-dynamically processed audio at small signal levels, for at least a portion of the low frequency range, the loudspeaker system and signal processor may provide the perception of high fidelity sound quality with the multi-modal processing being engaged mainly on greater amplitude, or, peak levels. And due to the multi-modal approach, the various aspects of the loudspeaker system and signal processor has the ability to maintain tonal quality and bass impact quality even on high dynamic range program material.

The application of taking signals from low frequency bands and transposing them to a narrow band or single frequency, may be improved with the support of at least one of a dynamic gain filter or fundamental enhancement by way of a harmonics generator over at least a portion of the low frequency range which may reduce a one note bass effect and may better maintain the tonal pitch of the original input signal from low to high signal levels.

Effective implementation of the example loudspeaker system and signal processor may be improved by having a frequency balance at small signal levels that is equalized to a preferred reference target curve for matching a reference sound quality and bandwidth, and then upon increasing level, using the interactive combination of signal processes and their match to the resonant chamber loudspeaker enclosure to substantially maintain a perception of that sound quality at large signal levels while minimizing audible overload distortion and eliminating damage to the loudspeaker.

It can be a further advantage of the embodiment illustrated in the graph 30 e of FIG. 7 (as compared to embodiment illustrated in graph 30 a of FIG. 3) that the diaphragm displacement sensitive frequency ranges 36 and 40 and dynamic filter gain reduction curves 36 b and 42 b may be even wider and deeper as transposing the gain-reduced energy to the tuning frequency is used to compensate for all gain/impact reductions, which can allow even greater perceived acoustic output without overload.

Signal processing block 22 in FIG. 1 and FIG. 6 may contain additional support processes to further enhance the primary dynamic signal processes. These may include additional fixed or dynamic gain filters or additional harmonic generators relating to any depressed amplitude frequency range. Additionally, the above mentioned processing blocks and threshold detector/activator 24 may incorporate one or more additional thresholds that may activate an overall dynamic high-pass gain filter process that may be engaged upon the audio signal levels reaching the transducer 18 driving the diaphragm 18 beyond a predetermined displacement limit to the point of being unable to be addressed by the primary processes or the audio signals being so large as to overdrive the transducer in the low displacement frequency range 32 or a range outside of that addressed by the primary processes discussed referring to FIG. 1 and FIG. 3 and FIG. 6 and FIG. 7. In the example system 10 b, the feedback path 21 may be applied to provide information from amplifier output/loudspeaker input point 21 a back to the threshold detector/activator 24. Alternatively a predictive model may be used that senses the input signal and includes information about a volume control setting and/or a gain profile of signal processing and the amplifier from input 23 to the amplifier output/loudspeaker input 21 a.

An organization of the control blocks in the example of FIG. 6 within signal processor 22 are such that the threshold detector/activator 24 is in series with, and ahead of, the following processor blocks of, the dynamic narrowband filter 25, the dynamic harmonic controller/generator 27, and the dynamic transpositional gain controller, the three of which operating in parallel, all being activated by the threshold detector/activator 24.

Alternatively, in other example systems, all the gain blocks in signal processor 22 could operate in series or a series/parallel combination, for instance, the threshold detector/activator 24 could activate the dynamic narrowband filter 25, which could serially activate both the dynamic harmonics controller/generator 27 and the dynamic transpositional gain controller 29 (operating in parallel with each other) upon a gain reduction being activated in the dynamic narrowband filter 25.

Still referring to FIG. 7, controlling the spacing 47 between the minimum diaphragm displacement frequency 34 a at fundamental resonant chamber resonance frequency F_(RC1) 34, and high diaphragm displacement frequency F_(MAX1) 37 a can impact the selection of parameters and optimization of relationships of between the multiple signal processes of signal processor 22 to maximize system performance. It has been found by the inventor that a frequency spacing ratio F_(SR1) of the maximum displacement frequency and the minimum displacement frequency spacing relationship that provides an effective configuration for the efficient functioning of the example processing, includes a frequency spacing value F_(SR1) determined by the ratio formula F_(MAX1)/F_(RC1)=F_(SR1), wherein the examples of the loudspeaker system with multi-mode signal processing are effective when the value of F_(SR1) is between 1.2 and 2.9, and other examples of the loudspeaker system with multi-mode signal processing are effective with a value be between 1.3 and 2.6, and a range of examples of the loudspeaker system with multi-mode signal processing are effective with an F_(SR1) value between 1.43 and 2.3. The more optimal spacing may provide combinations of system parameters to extend to a lower frequency capability, while allowing a reduction in enclosure volume, and still maintaining a fidelity of tonal quality and physical impact while minimizing audible overload distortion. These ratios can also apply to other examples of the loudspeaker system and signal processor besides the example of FIG. 6 and FIG. 7.

FIG. 8A represents one example of gain relationships of three dynamic processes, dynamic narrowband filter, dynamic harmonics generator, and dynamic transpositional gain controller, below, and above a level, or amplitude threshold. Graph 30 f has a vertical axis representing positive and negative gain change around a reference gain at zero, and the horizontal axis may correspond to an amplitude, in this case an amplitude of the signal output at terminal 21 a of the amplifier 20 which drives the diaphragm 64 displacement amplitude, within the narrowband frequency range 36 of FIG. 3 representing example system of FIG. 1, illustrated in this example for a dynamic narrowband filter and dynamic harmonics, and narrowband frequency range 36 of FIG. 7, representing example system of FIG. 6, illustrated in this example further including the dynamic transposed gain.

Again, describing the activity of the signal processor as discussed relative to previous drawings, and starting with reference to the example of the loudspeaker system and signal processor in FIG. 1 and the graph in FIG. 3, the non-linear gain of the dynamic processes are such that when the audio input signal, projected through any system equalization, signal path and amplifier gain profile are taken into account, while the loudspeaker system is operating in a smaller signal range 121, below threshold 122, the gain changes, shown in the vertical axis, of the dynamic processes are essentially dormant, or inactive.

As the threshold 122 is exceeded, with the system operating in the above-threshold operating-range 124, the threshold detector/activator 24 activates the dynamic filter gain 125, and in this example, the dynamic narrowband filter 25, activates a gain reduction that is further reduced in correspondence with further increases in a signal amplitude 120. Also, when the amplitude 120 exceeds threshold 122 into above threshold amplitude range 124, the dynamic harmonics generator 27 is activated creating harmonics in frequency range 39 to create a virtual fundamental tonal replacement gain increase 72 (shown in FIG. 4) in gain-reduced frequency range 36 corresponding inversely to the dynamic narrowband gain reduction. The activation of harmonics generation may correspond to the dynamically reduced gain 125 from the dynamic narrowband gain filter 25.

Now referring to the activity of the signal processor 22 as discussed relative to previous drawings, and starting with reference to the example of the loudspeaker system and signal processor in FIG. 6 and the graph in FIG. 7, in addition to the above description, relative to the example loudspeaker system and signal processor of FIG. 1, when the loudspeaker system is operating in the range 121 below threshold 122, the dynamic transpositional controller 29 may be essentially dormant, but, as the threshold 122 is exceeded, the dynamic transpositional gain controller 29 dynamically transposes a gain increase 127 to a minimized displacement frequency in the reduced displacement frequency range 32, corresponding to the gain reduction 125 of the dynamic narrowband filter in frequency range 36, the minimum displacement frequency preferably being that of resonant chamber resonance frequency 34.

The gain vs. amplitude graph 30 f may also represent other determiners of the threshold point, such as a voice coil thermal limit, a dynamic impedance change, an amplifier overload, or a passive acoustic radiator distortion limit, or a diaphragm displacement in another frequency range, such as a limited bandwidth frequency range, with one example being that of frequency range 40. Also, the non-linear effect of a dynamic process, such as the processes remaining inactive below the threshold level, and becoming active above the threshold level, may have a linear action or inter-process relationship, when above the threshold, or may deviate from a linear change or inter-process relationship above the threshold, as the system is optimized to maximize overload protection and maintain audio fidelity.

In various examples of the loudspeaker system and signal processor the threshold may be detected by detecting an amplitude level at an output from a point after amplifier 20. Alternatively, the threshold may be predicted from an analysis of an input audio signal by way of a predictive analysis of the gain profile of the signal path from an input signal to the loudspeaker transducer input.

FIG. 8B shows large-signal amplitude vs. frequency graph 30 g with maximum amplitude vs. frequency curve 45 representing the maximum acoustic output capability of transducer 18 in resonant chamber 16 enclosure 12 a relative to distortion limited maximum linear displacement capability of diaphragm 64. As an additional point of reference, the continued decline in output at low frequencies due to distortion limited maximum displacement when, unlike the loudspeaker system and signal processor disclosed herein, an enclosure type without a resonant chamber is used, such as an acoustic suspension enclosure, is represented by dotted line 45 a, which has even less bass capability than that shown in curve 44 a.

It can be seen that both frequency F_(RC1) 34 and the frequency 46 at the upper end of frequency band 36 are of similar amplitude and displacement. To use one example set of frequencies for illustration, the resonant chamber resonance frequency F_(RC1) 34 may be at approximately 40 Hz while frequency 46 may be about 2.5 times higher, at approximately 100 Hz, with displacement vulnerable frequency F_(MAX1) 37 a residing at approximately 1.5 times F_(RC1), or about 60 Hz. These relationships may be empirically scaled for optimization, depending on chosen enclosure and transducer parameters to optimize frequency spacings such that the multiple signal processes of signal processor 22 may interact effectively.

Because of the limited low output of the vulnerable displacement frequency 37 a, within the operational passband of the loudspeaker, the maximum output of the total usable passband without audible overload can be limited to displacement limited passband curve 44 a. By having the threshold detector/activator 24 triggering the dynamic narrowband filter 25 to reduce the gain in band 38 and filling in the gain-reduced fundamentals in band 38 with corresponding harmonics generated by dynamic harmonics generator 27, and maintaining full gain at tuning frequency F_(RC1) 34 with the loudspeaker system and signal processor the maximum output limitation is moved up to the maximum acoustic output level 44 b, which may be on the order of 6 to 12 dB greater than that of prior art systems with the displacement limited curve 44 a, without the combination of the resonant chamber enclosure and signal processing of the current loudspeaker system and signal processor. This increased capability can be achieved while keeping the perceived tonal response substantially maintained with harmonics generated by the harmonics generator 27 to fill in the tonal fundamentals in band 38 and maintaining perception of physical impact of the low frequencies by maintaining substantially full gain at physical impact frequency 34, which in a one preferred embodiment frequency 34 is in a range of 15 to 50 Hz and in another embodiment it may be between 50 and 80 Hz.

This system of using a loudspeaker enclosure with a resonant chamber with the disclosed signal processing of gain reduction of the second frequency band directly adjacent, and above, the first low displacement frequency band, coordinated with production of and gain increase of a dynamic harmonics generator, is not only beneficial to small systems in enhancing their ability to emulate larger bass systems, it is also very effective at increasing the output of large bass systems configured in the same manner. In large professional sound reinforcement systems, the larger displacement second frequency range 38 with large displacement frequency 37 a is the limiting factor, keeping the total system large signal levels to a maximum of displacement limited maximum acoustic output curve 44 a. By applying the techniques of the present loudspeaker system and signal processor, the large low frequency systems may have their large signal capability increased towards, or up to, an output the maximum acoustic output curve line 44 b, providing approximately a 6 to 12 dB of increased output, which is significant for any scale of audio system.

Referring to graph 30 g of FIG. 8C, as compared to the graph 30 e of FIG. 8A, the dynamic harmonics generator may deploy harmonics corresponding to a reduced level within a frequency range, such as frequency range 36, wherein a starting frequency response level that has a level depression falling below the target reference small signal reference frequency response, at least within a narrow bandwidth. In this approach the harmonics generator and/or the transpositional gain controller, may have a starting positive gain offset, as shown by dynamic harmonics gain curve 126 a, and dynamic transpositional gain curve 127 a, wherein curves 126 a and 127 a have a positive gain offset corresponding to a reduction in level in at least a narrow frequency range of the small signal response curve. This response curve may be inherently depressed in a low frequency range for a variety of reasons including being due to loudspeaker parameters that have other benefits, such as lower cost or reduced diaphragm displacement, desirable parameter tradeoffs, or greater upper range efficiency.

Referring to FIGS. 9, 9A, and 9B, FIG. 9 shows another type of resonant air-chamber enclosure 12 b with bass-reflex resonant chamber 16, passive acoustic mass radiator 14 a (shown here as a elongated vent or port) with transducer 18, including vibratile diaphragm 64. A second sealed, acoustic suspension air chamber 13, creating a bandpass response characteristic. The passive acoustic mass radiator may be an open vent or port, or may be a passive diaphragm radiator, as shown as 14 a in FIG. 6. The nature of the this enclosure type combined with the signal processing of the current loudspeaker system and signal processor can be expressed by the graph 30 c of FIG. 5, where in addition to the first dynamic narrowband filter 25, with gain reduction example shown as curve 36 b in secondary frequency range 36, a fourth frequency range 40 engages a second dynamic gain reduced filter curve 40 e or high-pass filter gain curve 40 e activity in frequency range 40. This approach is uniquely valuable to the enclosure type in FIG. 9, due to its pass-band continuing to realize efficiency and useful output well below first frequency band 32, wherein many of the other resonant chamber based enclosures of the loudspeaker system and signal processor disclosed herein, have significantly increased displacement be below tuning frequency F_(RC1) 34, and the lower frequency range audible amplitude falls at a rate below frequency range 32 at a rate of approximately 18 to 24 dB per octave.

FIG. 9A shows bandpass enclosure 12 c which is a variation on the enclosure of FIG. 9, with the main difference being that resonant chamber 16 can be reduced in volume and acoustical compliance in exchange for the passive acoustic radiator 14 g being longer and of greater acoustic mass than the passive acoustic radiator 14 c of FIG. 9. In the enclosure 12 c the vent 14 g may be of a length to operate also as a quarter wave-resonant air-column chamber forming an resonant chamber resonance independent of or supplemental to, the resonant chamber resonance of chamber 16, which may offer advantages particularly compatible with the resonant chamber and signal processor of the present loudspeaker system and signal processor, one of which may be more effective coupling to the transpositional gain controller transposing displacement gain to the resonant tuning frequency of enclosure 12 c.

FIG. 9B shows example enclosure 12 d, which is bandpass enclosure and part of a class of resonant chamber enclosures of the loudspeaker system and signal processor that incorporate more than one resonant chamber resonance frequency. Enclosure 12 d is similar to that of 12 c in FIG. 9, further including an additional bass-reflex resonant tuning chamber 16 b and passive acoustic radiator 14 d are added, which provide a second bass-reflex resonant tuning frequency. For multi-tuned resonant chamber systems, an example impedance curve graph 30 i is shown in FIG. 14A and an example diaphragm displacement curve graph 30 j is shown in FIG. 14B. This system also has the same feature as the enclosure of FIG. 9 of greater efficiency below the fundamental resonant chamber resonance frequency FRC1. An additional resonant chamber enclosure configuration (not shown) can be realized with the removal of sealed chamber 13, so that one surface side of the diaphragm 64 of transducer 18 radiates directly into the external environment, but the enclosure system still includes two resonant chambers 16 a, 16 b with two bass reflex tunings.

FIG. 10 shows resonant chamber based example enclosure 12 e, with bass-reflex resonant chamber 16, passive acoustic mass radiator 14 a (shown here as a elongated vent or port) with transducer 18, including vibratile diaphragm 64. Also included is a second bass-reflex resonant chamber 16 a, with a passive acoustic mass radiator 14 c (shown here as a vent or port) creating a dual-tuned, bandpass response characteristic.

FIG. 10A shows example resonant chamber based enclosure 12 f, configured as a bandpass enclosure with transducer 18 with diaphragm 64, with three bass reflex resonant chambers creating three tuning bass reflex tuning frequencies with resonant chambers; 16 a with passive acoustic radiator 14 c, and 16 b with passive acoustic radiator 14 d. The third bass reflex resonant chamber tuned to the lowest frequency of the three, creates a third chamber resonance with one of three possible vent/port passive acoustic radiator orientations, of 14 a or 14 e or 14 f.

FIG. 11 shows another type of resonant chamber enclosure 12 g with wave-resonant air-column 17, air-column mouth exit 15, with transducer 18, including vibratile diaphragm 64. This type of enclosure creates multiple resonant chamber wave based tunings at approximately ¼-wavelength relative to the length of air-column chamber 17, and each odd quarter wavelength thereafter. Wave-resonant air-column 17 may have a constant cross section area, or a positive taper cross section, expanding towards air-column mouth 15, or negative taper cross-section, contracting towards air-column mouth 15.

FIG. 11A shows example resonant chamber enclosure 12 h with resonant air-column 17, air-column mouth exit 15, with transducer 18, including vibratile diaphragm 64. This type of enclosure creates multiple resonant chamber wave based tunings at approximately ¼-wavelength relative to the length of wave-resonant air-column chamber 17, and each odd quarter wavelength thereafter. Additionally, the enclosure 12 h includes bass-reflex resonant coupling chamber 16 c.

FIG. 12 shows another type of resonant chamber enclosure 12 i with a regenerative wave-resonant air-column 17, air-column mouth exit 15, with transducer 18, including vibratile diaphragm 64. This type of enclosure creates multiple wave-resonant tunings at approximately ¼-wavelength relative to the length of resonant air-column chamber 17, and each odd quarter wavelength thereafter, creating a tapped or regenerative wave-resonant air-column waveguide. Wave-resonant air-column 17 may be constant cross section area, or expanding towards resonant air-column mouth 15 (as shown), or contracting towards resonant air-column mouth 15.

FIG. 13 shows still another type of resonant chamber enclosure 12 j with constricted 17 a center, wave-resonant air-column 17, with mouth flare 15 a at air-column mouth exit 15, and transducer 18, including vibratile diaphragm 64, coupled to flared throat 19. This type of enclosure creates multiple resonant tunings at approximately quarter-wavelength relative to the length of air-chamber 17, and each odd quarter wavelength multiple thereafter, with increased output capability at fundamental quarter-wave tuning frequency, F_(RC1).

With the above enclosure type embodiment examples of resonant-chamber based enclosures of the loudspeaker system and signal processor, a preferred element is that of exhibiting at least one, fundamental, low frequency resonant chamber tuning frequency F_(RC1) 34, with associated suppression of transducer diaphragm displacement, based on either a bass-reflex passive-mass/air-volume-compliance chamber resonance or a wave-resonant, air-column wavelength based resonance in an elongated waveguide, pipe, transmission-line or horn. The enclosure may further include variations including but not limited to examples of; bass reflex, Helmholtz-reflex, bandpass enclosures, each including a passive acoustic radiator, such as a vent, port, or passive acoustic diaphragm, and air-column based air chambers, including but not limited to examples of a quarter wave pipe, horn, tapped horn, inverse-horn, tapped/regenerative waveguide, Voigt pipe, or other resonant chamber systems with an associated transducer diaphragm displacement minimum, or a combination of one or more of the above enclosure types.

FIG. 14A shows graph 30 i, illustrating enclosure/transducer impedance curve 31 f, corresponding to multi-resonant enclosures, such as shown in FIGS. 9B, 10, 10A, 11, 11A, 12, and 13, wherein an impedance minimum 31 b corresponds to a lowest, fundamental, resonant chamber resonance frequency F_(RC1) 34 in first frequency range 32. Transducer resonance impedance peak 31 a may be within frequency range 40 or at the lower frequency portion of frequency range 32, and transducer impedance peak 31 c may fall within second frequency range 36 or may be at a somewhat higher frequency, in frequency range 39.

The next impedance minimum 31 d, above impedance peak 31 c, is that of a second diaphragm displacement minimum, resonance frequency 34 c, F_(RC2) in second reduced diaphragm displacement frequency range 32 a, followed by transducer impedance peak 31 e in frequency range 48 and broader frequency range 39.

Resonant chamber based loudspeakers of the loudspeaker system and signal processor, including resonant bass-reflex and wave-resonant air-columns, exhibit at least one chamber resonance causing the loudspeaker system 10 to exhibit a fundamental resonant chamber resonance frequency 34 at a low operating frequency range where the diaphragm displacement as a function of frequency is minimized as opposed to a, non-resonant chamber based enclosure, such as an acoustic suspension or open baffle for which there is no resonant chamber resonance or diaphragm displacement minimum as a function of frequency, and transducer diaphragm motion is increased for all low frequencies.

FIG. 14B is a diaphragm displacement vs. frequency chart 30 j showing the displacement response shape of the first two lowest frequency resonant chamber resonance modes that corresponds to operation of multi-tuned bass-reflex, and wave-resonant air-column enclosure examples shown in FIGS. 9B, 10, 10A, 11, 11A, 12, and 13. It can be seen that there are two frequencies of diaphragm displacement minimums 34 a and 34 d, at resonant chamber, resonant frequency resonances of F_(RC1) 34 and F_(RC2) 34 c. As another example approach to the loudspeaker system and signal processor, resonant chamber resonance frequencies F_(RC1) 34 and/or F_(R2) 34 c, may be used as a dynamic transpositional target frequency and may depend on which is closest in frequency or harmonic relationship to a dynamic gain reduced frequency. This may work well particularly if the system is arranged to operate at very low frequencies, such that F_(RC2) is preferably below 70 Hz and F_(RC1) is at a an even lower frequency. Graph 30 j also shows additional increased diaphragm displacement frequency range 48 with additional displacement maximum frequency 37 c and a potential additional application of dynamic narrowband gain reduction as in illustrative example curve 48 b, for which in a one preferred embodiment there may also be a correspondingly generated dynamic harmonics for frequency range 48 upon dynamic gain reduction 48 b and in another preferred embodiment, a transpositional gain controller may be applied to transpose an increase in gain in frequency range 32 or frequency range 32 a as replacement gain for gain reduced frequencies in frequency range 48. Frequency ranges, filter gain curves, and displacement curves below frequency range 32 a are essentially the same as those discussed for FIG. 5, as are the applications of the multi-modal signal processes, gain filters, harmonic generators and controllers, and transpositional gain controllers. The systems of this type of multiple resonant chamber resonance frequencies with multiple diaphragm minimum frequencies may work better for improving low frequency capability in larger systems, or systems that are operating in the lower frequency ranges, such as extending downward in frequency to include at least some portion of the frequency ranges from below approximately 20 Hz to 70 Hz, where larger cubic volume displacements may be required.

Loudspeaker system 10 c of FIG. 15 shows another example of the loudspeaker system and signal processor with low frequency signal processing 22, including resonant chamber enclosure 12 a, woofer transducer 18, including a vibratile diaphragm 64. The loudspeaker enclosure 12 a further includes at least one bass-reflex resonant chamber 16, and passive acoustic mass radiator 14 b, shown here as a passive diaphragm radiator, but can optionally be interchanged with a vent or port, as shown in FIG. 1 as 14 a. The transducer 18 is driven by amplifier 20 and connected to the input of the amplifier 20 is the multi-mode signal processor block 22, including threshold detector/activator 24, dynamic narrowband filter 25, and transpositional gain controller 29.

Referring to loudspeaker system 10 c in FIG. 15 and graph 30 e of FIG. 15A, at small signal levels, the dynamic processes of the processing block 22 may remain substantially dormant until an audio input signal, received by audio input 23, and amplified to output 21 a by amplifier 20, increases to a level where an amplitude threshold is reached, upon which the threshold detector/activator 24 activates the dynamic narrowband filter 25 to reduce gain incrementally as a smooth or incremental gain change filter, or in a gain stepped manner, as a gain step gain change filter, with gain steps (as one fully gain reduced curve is represented in curve 36 b) in a second frequency range 36, which is adjacent to, and above, a first frequency range 32, which contains resonant chamber resonance tuning frequency 34. There may be limited to a an asymmetrical step process with a single step to maximum gain reduction and a multiple steps of recovering gain back to zero gain reduction, or a symmetrical step process with one step between minimum and maximum gain reduction or multiple gain steps of approximately 2 to 6 dB per step of gain reduction to maximum gain reduction and multiple steps in gain recovery back to zero gain reduction in frequency range 36. The stepped and incremental approaches described above may be applied to other example dynamic processes and filters of signal processor 22.

Upon the onset of gain reduction in frequency band 36, the dynamic transpositional gain controller 29 is activated wherein frequencies within band 36 that are gain reduced as shown in gain reduction curve 36 b, have at least a portion of the magnitude of their gain reduction, transposed to a frequency at, or near, the diaphragm displacement minimum 34 a resonant chamber frequency 34 within first frequency band 32 with a gain boost example 34 b at the resonant chamber 16 tuning frequency 34 corresponding to the gain reduction 36 b of frequencies in frequency band 36. The transposed gain replacement of gain reduced frequencies of frequency 36 is balanced such that the perceived physical impact fidelity of frequency range 36 after gain reduction sustains a perception of preferred physical bass impact or may correspond to a perceived physical impact fidelity below threshold levels prior to any gain reduction of frequency range 36.

Frequency range 40 may include gain reduction filters creating gain reduced curves 42 b or 42 c reducing gain from the non-gain reduced curve shown as 42 a. The gain reduction filter in frequency range 40 may have a curve shape that is may be one or both of a high-pass filter and a narrowband filter, and the gain reduction filter for frequency range 40 may also have an activation type to be a fixed gain filter or a dynamic gain filter. As a dynamic gain filter operating in frequency range 40, there may be an incremental gain reduction or alternatively, a stepped gain reduction, with a singular step or there may be multiple steps of approximately 2 to 6 dB per step of gain reduction in frequency range 40.

Optionally or alternatively, as a predetermined secondary band limited amplitude threshold is reached for frequencies in frequency range 40 creating as an illustrative example, narrowband gain reduction curve 42 b or high-pass gain reduction curve 42 c, those frequencies and gain corresponding to the amount of reduced gain is dynamically transposed to a frequency of the displacement reduced frequencies in the first frequency range 32, preferably to resonant chamber resonance frequency F_(RC1), 34 with transposed frequency gain illustrated as 34 b. The supplemental process for the gain-reduced frequencies of the fourth frequency range 40 may be the transpositional gain controller and the transpositional gain controller may be one of a static transpositional gain controller and a dynamic transitional gain controller. The dynamic or static nature of the transpositional gain controller may be determined by whether the operational nature of the band limited gain filter in the frequency range 40 is a dynamic or a fixed (or static) gain filter, with it being preferable for the operational aspect of the filter to match that of the transpositional gain controller in onset and release, and also to inversely match that of the transpositional gain controller in relation to a gain change in frequency range 40.

It may be advantageous to utilize the transpositional gain controller of one or more of the loudspeaker system and signal processor examples to transpose a gain of at least a portion of a diminished amplitude level as a function of frequency that may occur at any of the low frequencies, particularly below 100 Hz, and preferably below 70 Hz, with that gain being transposed to a frequency of reduced diaphragm displacement, to augment a physical impact gain that is lost while minimizing a perception of audible overload of the loudspeaker system, with a tradeoff of overload distortion and perception of physical bass impact being balanced for best overall perceptual performance.

It is perceptually advantageous that the use of transposing the gain of bass frequencies be accompanied by an additional signal process, such as the dynamic gain filter, to maintain perceptually accurate tonal balance at all signal levels and to override the ear's ability to have the pitch of the transpositional frequency impact the perceived pitch over that of the gain reduced frequencies. It also may be a perceptually advantageous feature the loudspeaker system and signal processor, that the dynamic transpositional gain controller 29 is dynamic, when used with the dynamic gain filter, meaning that it may be dormant and essentially not functional at small signal levels below the amplitude threshold levels. This can be significant with most program material, that most, or all, of the dynamic processes of the signal processing block can be inactive at small signal and/or average level program material, maintaining a low coloration, high fidelity sound quality equivalent to that of a much larger, high quality system without the present loudspeaker system and signal processor, and preferably only activating the multiple signal processing modalities at higher levels, using the interactive modes to maintain, the tonal quality and physical bass impact while being able to increase total system sound pressure levels while effectively minimizing audible overload distortion.

The psychoacoustics of the ear-brain system may establish a large portion of its judgment about a sound based on the sustained average levels, often as much, or even more than the instantaneous peak levels. By maintaining the original, non-dynamically processed audio at small signal levels, for at least a portion of the low frequency range, the present loudspeaker system and signal processor may provide the perception of very high fidelity sound quality with the multi-modal processing being engaged mainly on greater amplitude, or, peak levels. And due to the multi-modal approach, the various aspects of the loudspeaker system and signal processor provide the ability to maintain tonal quality and bass impact quality even on high dynamic range program material.

The application of taking signals from low frequency bands and transposing them to a narrow band or single frequency, may be best deployed with support of at least one additional mode of the multi-mode signal processor, such as incorporating a dynamic gain filter over at least a portion of the low frequency range to avoid the sonic effect of what is known to be experienced as “one note bass” to more effectively maintain the tonal pitch and physical impact fidelity of the original input signal at low levels or high signal levels.

Effective implementation of the loudspeaker system and signal processor may be improved by having a frequency balance at small signal levels that is equalized to a preferred reference target curve for matching a reference sound quality and bandwidth, and then upon increasing level, using the interactive combination of signal processes and their match to the resonant chamber loudspeaker enclosure to substantially maintain a perception of that sound quality at large signal levels while minimizing audible overload distortion and eliminating damage to the loudspeaker.

It can be a further advantage of the embodiment illustrated in the graph 30 e of FIG. 15A (as compared to embodiment illustrated in graph 30 a of FIG. 3) that the diaphragm displacement sensitive frequency ranges 36 and 40 and dynamic filter gain reduction curves 36 b and 42 b may be even wider (and may even extending somewhat into frequency range 39) and deeper as transposing the gain-reduced energy to the tuning frequency is used to compensate for all gain/impact reductions, which can allow even greater perceived acoustic output without overload.

As an optimizing coordination of the enclosure system 12 a parameters, with the multi-modal processes of signal processor 22, the frequency range 47, representing a difference in frequency between diaphragm displacement minimum frequency 34 a, of resonant chamber resonance frequency F_(RC1) 34, and a maximum displacement frequency F_(MAX1) 37 a, it can be advantageous for the frequency spacing ratio F_(SR1)=F_(MAX1)/F_(RC1) to have a value F_(SR1) of between 1.2 and 2.9. It can be effective for a range of examples of the loudspeaker system with multi-mode signal processor for the frequency spacing ratio F_(SR1) to be between 1.3 and 2.6, for some example systems, including some larger example enclosure systems, or fourth order Butterworth bass-reflex enclosure alignments, whereas some example systems, including the smaller system examples with low frequencies more extended for a given enclosure volume may be more advantageously optimized for maximum low frequency extension and capability and compatibility with the signal processes of signal processor 22, when the frequency spacing ratio F_(SR1) is between 1.43 and 2.3. These same ratio values may also be applied advantageously to the other examples of the loudspeaker system disclosed herein.

Signal processing block 22 in FIG. 1 and FIG. 6 and other examples of the signal processing block 22 of the loudspeaker system may contain additional support processes to further enhance the primary dynamic signal processes. These may include additional fixed or dynamic gain filters or additional transpositional gain controllers relating to any depressed amplitude, or gain reduced frequency range. Additionally, the above mentioned processing blocks and threshold detector/activator 24 may incorporate one or more additional thresholds that may activate an overall dynamic high-pass gain filter process that may be engaged upon the audio signal levels reaching the transducer 18 driving the diaphragm 18 beyond a predetermined displacement limit to the point of being unable to be addressed by the primary processes or the audio signals being so large as to overdrive the transducer in the low displacement frequency range 32 or a range outside of that addressed by the primary processes discussed referring to in the examples FIG. 1 and FIG. 3 and FIG. 15 and FIG. 15A or other examples of the loudspeaker system and signal processor. If an audio input signal is so high in amplitude as it appears at the amplifier 20 output 21 a that, even low displacement frequency range 32 may start to overload, an example of the loudspeaker system with processor may include a full frequency range gain reduction or additional gain reduction filtering that may be applied such that a narrowband filter, a high-pass filter, or a shelving filter may be activated for gain reduction over a frequency range that includes frequency range 32, to minimize audible overload distortion in the loudspeaker system.

In the example system 10 c, the feedback path 21 may be applied to provide information from amplifier output/loudspeaker input point 21 a back to the threshold detector/activator 24. Alternatively a predictive model may be used that senses the input signal and includes information about a volume control setting and/or a gain profile of signal processing and the amplifier from input 23 to the amplifier output/loudspeaker input 21 a.

A fourth example of the loudspeaker system and low frequency signal processor 10 d in FIG. 16 comprises loudspeaker enclosure system 12 a including resonant chamber 16 and passive acoustic mass radiator 14 b, to form a bass-reflex resonant chamber enclosure, incorporating transducer 18 with diaphragm 64. Further included is signal processor 22, including threshold detector/activator 24 a, harmonics generator/controller 27 a and transpositional gain controller 29 a.

Referring to FIG. 16 and FIG. 16A, the system 10 d may have a predetermined, reference target response curve 35 b, but does not meet the preferred amplitude level, as shown by amplitude depression 36 c, with differential amplitude loss 36 d, and amplitude depression 40 f, with differential amplitude loss 40 g. A threshold detector/activator 24 a may be utilized to detect a minimum differential amplitude loss, with an example as greater than 2 dB, and activating at least a partial corrective action from the harmonics generator and/or transpositional gain controller. Alternatively, the system may operate without a threshold detector/activator, by having these corrective actions of the harmonics generator and/or transpositional gain controller but preset at the time of system design or assembly. For amplitude depressions 40 f and 36 c the harmonics generator may generate harmonics 74 that correspond to at least a portion of the amplitude loss of fundamental frequencies within frequency ranges 36 and 40, creating virtual frequency gain 72 and 72 a to tonally replace at least a portion of the amplitude differential losses 36 d and 40 g to regain a perceived tonal balance closer to that of the target reference curve level 35 b. Additionally, for amplitude depressions 40 f and 36 c the transpositional gain controller may generate and transpose at least a portion of the amplitude differential losses 36 d and 40 g to a low displacement frequency range 32 and may transpose the gain to resonant chamber resonance F_(RC1) 34 of that corresponds to at least a portion of the amplitude loss of fundamental frequencies within frequency ranges 36 and 40, creating physical impact transposed gain 34 b to replace at least a portion of the amplitude differential losses 36 d and 40 g to regain a perceived physical impact balance closer to that of the target reference curve level 35 b.

FIG. 16A shows gain and harmonics generation in amplitude/gain level graph 30 o showing frequency range 36 and frequency range 36 being represented with level reduced frequency curve example 36 c. Frequency 34 shows chamber fundamental, resonant chamber resonance tuning frequency F_(RC1). When frequency range 36 has reduced level 36 c, as a frequency response error, or a pre-equalized setting to minimize diaphragm 64 displacement in high displacement frequency range 36, the harmonics generator produces harmonic series 74 in frequency range 39, including harmonics, 74 a, 74 b, 74 c, (74 d representing more or less included harmonics as they may be even or odd harmonics or a mix of both and may be carried up to a higher harmonic count or limited to just the lower harmonics first, second, third, and may be attenuated with each increasing harmonic number) creating perceived, virtual fundamental frequency 72 at reference target level 35 b and 36 a as the harmonics create a psycho-acoustic, virtual pitch 72 representation of the reduced level fundamental frequencies in curve 36 c which is perceived by the listener as substantially the same tonal character and tonal level as the target amplitude level 35 b in frequency range 36 and it is perceived at substantially full gain level 36 a, creating a virtual fundamental 72, tonally duplicating the fundamental as if it was not level reduced. This can be applied to one or more level reduced fundamentals frequencies in the frequency range 36.

This balance of having the level reduced in frequency range 36 as a frequency response error or limitation of the loudspeaker system or to protect from audible overload distortion, and the harmonics in frequency range 39 having a corresponding gain increase to create virtual tone replacement frequencies 72 may substantially regain and maintain the perceived tonal balance of the loudspeaker system while allowing the system to operate at much greater output levels while minimizing audible overload distortion. Also, by maintaining the system gain at frequencies in frequency range 32, much of the perceived physical impact from reproduced bass frequencies is preserved such that the system minimizes overload distortion while playing louder, while sustaining tonal and physical impact fidelity.

The dynamic harmonics generator 27 may operate effectively for a given gain suppressed frequency band of two octaves or less, and in some examples when creating a virtual tonal replacement of approximately 1.5 octaves or less, and therefore the bandwidth of the dynamic narrowband filter may be effective when realizing a maximum bandwidth of two octaves, and in some examples of the loudspeaker system and signal processor, approximately 1.5 octaves or less, and to have the narrowband level reduction bandwidth 36 c and the harmonics generator virtual fundamentals 72, within frequency range 36, have a bandwidth that substantially matches the level reduced bandwidth 36 c. Beside the bandwidths corresponding between the narrowband level depression and the virtual tones of the harmonics generator, the level reduction of the narrowband depression and the gain increase of the generated harmonic series 74, may have a corresponding inverse gain relationship to have the tonal effect of the narrowband level reduction 36 c be effectively, perceptually replaced by the perceived level of the virtual tone or tones, 72.

FIG. 17 represents a fifth example 10 e of the inventive loudspeaker system similar to that shown in FIG. 6 and with a variation of the signal processing blocks, filter gain controller 25 a and frequency generator block 28 including dynamic harmonics generator 27 and dynamic transpositional gain controller 29. The filter gain controller 25 a may include a dynamic narrowband filter 25 (as shown in FIG. 1 and FIG. 6) and may also include additional dynamic gain filters with one example of frequency curves illustrated in FIG. 5 as dynamic gain high pass example curve 40 d and additional dynamic narrowband filter shown as an example curve 40 e. The filter gain controller block 25 a may also include a fixed target response equalization and fixed amplitude suppression filters such as example high-pass filter curve 40 b or narrowband filter 40 c, shown in FIG. 3, and the signal processing block 22 may also include other supporting, ancillary processes such as transpositional gain controller 29 to transpose gain from any gain reduced, increased diaphragm displacement frequency range to a reduced diaphragm displacement frequency range to maintain system performance at very high signal levels and high amplitudes in any frequency band, as disclosed for the signal processing in FIG. 1 and FIG. 6. The more generalized adaptive signal processing of this example 10 e loudspeaker system processing may work effectively to maximize the performance the different versions the resonant chamber enclosures disclosed, driven from amplifier output/loudspeaker input 21 a.

The frequency generator block 28 may perform as a signal generator of frequencies not appearing in the input signal and may generate either a set of harmonics for the dynamic harmonics generator 27 or operate as a signal generator to generate a signal at, at least one frequency, and provide gain control at that frequency, as the transpositional target frequency for the dynamic transpositional gain controller 29, such as resonant chamber resonance frequency 34. The dynamic gain filter system may include a dynamic narrowband filter 25 (shown in FIG. 1 and FIG. 3 frequency range illustrative example curve 36 b) or a number additional or optional gain filters, such as one or more of a dynamic high pass gain filter, a fixed gain high pass filter, a fixed gain narrowband filter, additional dynamic narrowband gain filters, or other supporting filter processes. The processed signal result of the dynamic gain filter system 25 a, dynamic harmonics generator 27 and the dynamic transpositional gain controller 29 may sum together at summing/mixing junction 21 b. The processing block preferably engages at least a dynamic gain filter system 25 a, and a dynamic harmonics generator 27 and a threshold detector/activator 24, but in some embodiments may engage at least two of a dynamic gain filter system 25 a, a dynamic harmonics generator 27, a threshold detector/activator 24 and a transpositional gain controller 29. FIG. 17 shows amplifier 20 and loudspeaker enclosure 12 a with resonant air-chamber 16 and transducer 18 with vibratile diaphragm 18 and passive acoustic radiator 14 b, as described in FIG. 6, but any of the previously disclosed enclosure types may be substituted for that of 12 a in alternative embodiments.

FIG. 18 represents a sixth example 10 f of the loudspeaker system and signal processor, including bandpass enclosure 12 b with a resonant chamber 16 with passive acoustic radiator 14 c, sealed chamber 13, incorporating transducer 18 with diaphragm 64. Also included is signal processor 22 with threshold detector/activator 24, pre-equalizer 80, dynamic narrowband filter 25, dynamic harmonics controller/generator 27, dynamic high-pass filter 25 a, and optional dynamic transpositional gain controller 29. Processor 22 drives amplifier 20 to output 21 a, with feedback signal line 21 routing back to threshold detector/activator 24. Pre-equalizer 80 provides a small signal fixed equalization curve to match a target reference frequency response curve, for example reference target curve 35 b in FIG. 2 or any preferred starting, or below threshold, amplitude curve. Pre-equalizer can be connected directly to the input 23 with a threshold detector 24 pass-through connection, such that the pre-equalized signal is what the threshold detector responds to, be it directly to the threshold detector 24, feedback optionally from pre-equalizer by way of feedback line 21 or by way of feedback line 21 feeding a pre-equalized signal from the amplifier output signal 21 a back to the threshold detector/activator 24.

As the pre-equalizer 80 may operate ahead of, or feed back to, the threshold detector 24, the output of the threshold detector/activator 24 can connect serially to activate substantially simultaneously, the dynamic narrowband filter 25, dynamic high-pass filter 25 a, dynamic harmonics controller/generator 27, and the optional dynamic transpositional gain controller, of which all three operate in parallel but, alternatively, in some example systems, can operate in series or in a series/parallel combination.

Referring also to graph 30 e in FIG. 7, the dynamic narrowband filter 25 operates as discussed relative to the FIG. 1 and FIG. 6 systems with a predetermined amplitude threshold level activating the dynamic narrowband filter 25 reducing a narrowband gain in frequency range 36 and simultaneously applying dynamic harmonics generation in frequency range 39 to replace the narrowband gain with a corresponding virtual tone gain derived from the harmonics generated in frequency range 39. Additionally, dynamic high-pass filter 25 a in response to the threshold detector/activator assessment of a diaphragm 64 displacement overload threshold being reached for the limited bandwidth frequency range 40, with representative gain reductions of the high-pass filter being represented by reduced gain curve 42 c. For the gain reduced fundamental frequencies in frequency range 40 corresponding harmonic frequencies may be generated by the dynamic harmonics controller/generator 27 to create at least a partial virtual fundamental gain replacement for the gain-reduced frequencies to restore their tonal balance after gain reduction. Optionally, the dynamic transpositional gain controller 29 may produce a transposed gain 34 b corresponding to at least a portion of the gain reductions 36 b in frequency range 36 and 42 c in frequency range 40, and transpose at least a portion of those reduced gains to generate a tonal gain at a gain reduced displacement frequency in frequency range 32, preferably at diaphragm minimum 34 a at chamber resonance frequency F_(RC1) 34.

FIG. 19 represents a seventh example 10 g of the loudspeaker system and signal processor, wherein the loudspeaker system includes a low frequency woofer system enclosure 12 b with transducer 18 with diaphragm 64, bass-reflex resonant chamber 16 with passive acoustic radiator 14 c and sealed, acoustic suspension chamber 13. Also including in this example loudspeaker system is an upper frequency system enclosure 12 k, with upper range transducer 18 a including diaphragm 64 a, loaded into resonant chamber 16 e with passive acoustic radiator 14 h. The upper frequency enclosure system may, in an alternative version, utilize a non-resonant chamber based enclosure or baffle, such as an acoustic suspension, sealed chamber enclosure, or an open baffle.

The loudspeaker system signal processor block 22 includes signal input terminal 23 adapted to receive an electrical input signal, threshold detector/activator 24, low-pass filter 80 a, dynamic gain band filters 25, dynamic harmonics generator 27, high-pass filter 82, and optional dynamic transpositional gain controller 29, amplifier 20, and upper frequency amplifier 20 a. The signal processing block 22 includes high pass filter 82 to create a high pass input to amplifier 20 a and upper frequency range enclosure 12 k to attenuate low frequencies and cross over to the lower frequency enclosure system 12 b. The low pass filter has at least one function to create a low pass crossover characteristic to attenuate the upper frequencies of the lower frequency enclosure 12 b to cross over in a manner that matches the upper frequency enclosure system 12 k with a smooth transition. Also, feedback loop 21 may feedback displacement information from amplifier output 21 a to the threshold detector/activator 24.

Referring to example loudspeaker system 10 g of FIG. 19, and also the corresponding graphs 30 k in FIG. 20, 30 l in FIGS. 21, and 30 m in FIG. 22, it may be advantageous to utilize a second transducer or a second loudspeaker enclosure to realize the loudspeaker system and signal processor, such as when a bandpass woofer enclosure system 12 b may not have the upper frequency bandwidth to produce the generated harmonics adequately to support the gain reduced frequencies, such as those in frequency range 36, or if there may be an opportunity to have the generated harmonics maintain greater dispersion by assigning at least a portion of them to smaller transducer 18 a or sound source, or there may be directionality or spatial sonic imaging issues that allow the harmonics to be generated while not disturbing the spatial and tonal integrity of the total loudspeaker system. It may also be advantageous to have the harmonics appear in another diaphragm displacement reduced frequency range of another transducer or loudspeaker enclosure with an enclosure with a resonant chamber resonance, such as enclosure 12 k, resonant chamber 16 e with passive acoustic radiator 14 h, with a diaphragm 64 a displacement minimum 34 d which may more easily support the increased gain applied to the generated harmonics. There may be other advantages from deployment of the generated harmonics in the operational range of a transducer 18 a that is separate from the primary transducer 18, as shown in this example, enclosure 12 b.

As one example, it can be seen in graph 30 k of FIG. 20, that the bandwidth of diaphragm displacement curve 41 a falls in amplitude with a low pass characteristic immediately above frequency range 36 which would make it difficult to provide extended harmonic support in a frequency range 39. By including an upper frequency transducer or loudspeaker enclosure system, such as 12 k in FIG. 19, it can be seen in graph 30 k that the diaphragm displacement curve 41 b, representing the diaphragm 64 a displacement of transducer 18 a in the enclosure system 12 k, can extend into frequency range 39 to effectively reproduce the generated harmonics from dynamic harmonics generator 25 that would desirably appear in frequency range 39 to support a gain reduced frequency curve 36 b with virtual fundamental frequencies corresponding to the harmonics generated in frequency range 39 and corresponding to gain reduced frequencies in frequency range 36. In some cases the supporting, generated harmonics, may support a gain reduction frequency range 40, and at least a portion of those supporting harmonics may be placed in frequency range 39, and produced by transducer 18 a in loudspeaker enclosure 12 k. It can be seen that the diaphragm 64 a displacement curve 41 b for enclosure system 12 k has a resonance frequency diaphragm displacement minimum of 34 f at bass-reflex, resonant chamber resonance frequency F_(RC1S) 34 e.

With the system operating as with the previously described operational attributes in previous examples, such as that of FIG. 1 and FIG. 3, as a narrowband amplitude threshold is reached in frequency range 36, that contains a maximum excursion frequency F_(MAX1) 37 a, the gain is reduced in frequency range 36 to avoid audible overload distortion by way of gain reduced curve 36 b, and at the same time the dynamic harmonics generator 27, generates harmonics in frequency range 39, corresponding to gain reduced frequencies in frequency range 36, such that virtual fundamental frequency tonal replacement gain is produced in frequency range 36.

It can be seen in curve 41 c in FIG. 21 amplitude/gain level vs. frequency graph 30 l, representing lower frequency enclosure system 12 b of FIG. 19, that the gain is upheld at resonance frequency F_(RC1) 34 and gain has been reduced in frequency range 36, as shown by curve 36 b, and virtual gain replacement frequency 72 appears in frequency range 36 to replace the tonal characteristic of the gain reduced frequencies substantially back to the pre-threshold, pre-gain reduced, and desired tonal amplitude level 36 a. Curve 41 c in the frequency range 39 is shown to attenuate significantly in the range where the generated harmonics 74 are desirably reproduced, and those harmonics (other than possibly the first harmonic 74 a) may not be developed at sufficient amplitude to create the desired level of virtual fundamental frequency 72 in frequency range 36. In amplitude/gain level vs. frequency graph 30 m in FIG. 22, representing upper frequency enclosure system 12 k of FIG. 19, it can be seen that amplitude curve 41 d, representing the upper frequency enclosure system 12 k has a full amplitude extended range through frequency range 39 to adequately reproduce the full gain of the generated harmonics 74 to create the virtual frequency 72 at the desired amplitude level to support gain reduced frequencies in frequency range 36 of enclosure 12 b.

The example of the loudspeaker system and signal processor shown in FIGS. 19, 20,21, and 22 may be realized with various alternate combinations, including a separate, upper range transducer added to the primary enclosure 12 b, the use of a non-resonant chamber based enclosure for the upper range enclosure system 12 k, and primary lower range enclosure 12 b may be of any enclosure including at least one resonant chamber that is one of a bass-reflex resonant chamber and a wave-column resonant chamber. Additionally, it is possible to realize the concept with separate upper and lower frequency transducers with a single amplifier and passive high-pass and low-pass crossover filters. Further, the transpositional gain controller 29 may be optionally added as discussed in previous examples.

FIG. 23 represents another example 10 h of the loudspeaker system and processor, wherein as a variation on the example illustrated in FIG. 1, and in other processor architecture examples of the loudspeaker system and signal processor, the dynamic narrowband filter 25 and dynamic harmonics generator 27 may operate in a manner, wherein the dynamic filter operates as a real-time dynamic filter 25 b with an instantaneous gain reduction at threshold triggered by the threshold detector/activator 24 and an instantaneous gain recovery release, substantially at the audio signal rate, upon the audio signal falling in level below the threshold level, or essentially as a real-time gain control filter at the audio rate. In this fast onset/fast release approach the dynamic narrowband filter 25 of FIG. 1 may operate in the example 10 h as a dynamic real-time gain filter 25 b, wherein some desired harmonics, generated only by the dynamic harmonics generator 27, of FIG. 1, may be generated by the dynamic real-time gain filter 25 b, so the dynamic harmonics controller 27 b may shape or cancel or generate harmonics to end up with a complimentary set of harmonics that add to or cancel or shape the harmonics generated by the fast release time of the dynamic real-time gain filter 25 b to have the resultant harmonic series and harmonic amplitude relationships be the desired combination to create the appropriate tonal replacement for the gain reduced fundamental frequencies in a gain reduced frequency band, such as narrowband frequency range 36 of FIG. 3. To generate the optimal harmonic series, the dynamic harmonics controller 27 a may operate with the same attack and release time of the dynamic real-time gain filter 25 b or with an altered attack and release time to most effectively compliment the dynamic real-time gain filter 25 b. As with all forms of the harmonics generated there may be additional processing to shape and form the correct level and relationship of the harmonic series. The real-time dynamic filter and harmonics controller by having substantially instantaneous release time can shorten the time that a gain reduced frequency range will remain suppressed, which in some configurations of the loudspeaker system and signal processor may improve the perceived tonal and impact fidelity by eliminating recovery lag times. The dynamic real-time processing of dynamic gain filter, such as a dynamic narrowband gain filter or dynamic high-pass gain filter, may also include additional dynamic real-time associated processing, such as dynamic transpositional gain processing as disclosed in previous examples. The transpositional gain controller may also adopt the real-time onset and release time when used with the real-time dynamic gain filter. With the potential improvement in some examples of the loudspeaker system and processor by use of real-time processing recovery it may be important to optimize any distortion artifacts or harmonics generated by the instant recovery time, by shaping, cancelling or adding to the harmonics, to create the optimal amount of harmonics energy or a harmonic series with a similar perceptual tonal effect of harmonics generated independently by the dynamic harmonics generator/controller of the example in FIG. 1. Therefore, in an example loudspeaker and signal processor of the type shown in FIG. 23 the harmonics controller controls a real-time attack time and release time distortion and optimizes resultant harmonics and minimizes audible distortion artifacts by at least one of shaping, cancelling and adding to, a harmonic distortion produced by the real-time dynamic gain filter, in some examples of the loudspeaker system and processor, may be a dynamic narrowband filter.

As with the non-real-time dynamic gain filter examples of the loudspeaker system and signal processor, this real-time processing example may be used with the various filters contours, such as a narrowband filter, a shelving filter, or a high-pass filter, or some combination there of, and may be used singly, for one frequency range, such as the narrowband frequency range 36, or band limited frequency range 40, or with multiple real-time processing filters working in multiple frequency ranges on the same loudspeaker system. The real-time processing 22 a may also be applied to the bass reflex resonant chamber enclosure 12 as shown with bass reflex resonant chamber 16, passive acoustic radiator 14 a, and transducer 18, with diaphragm 64, or with any of the enclosure systems with at least one resonant chamber resonance. Real-time processor 22 a may receive a feedback signal from amplifier 20 output 21 a to establish when the threshold level has been reached, or may have a predictive, feed-forward signal for determining the when the predetermined threshold level has been reached, where in the feed forward signal is the input signal calibrated by the gain profiles of the signal processor 22 a and amplifier 20.

In one example loudspeaker system and signal processor, shown in FIG. 23, the operational organization of gain blocks in signal processor 22 a may start with threshold detector/activator 24 operating in series with the dynamic real-time gain filter 25 b, activating the dynamic real-time gain filter 25 b upon the amplitude threshold being exceeded, and the dynamic harmonics controller 27 b serially follows the dynamic real-time gain filter 25 b to supplement, cancel, or shape distortion harmonics that are produced by the dynamic real-time gain filter 25 b wherein the output of the dynamic harmonics controller 27 b is directed to the amplifier 20. Optionally, the dynamic transpositional gain controller may be triggered by activation from the threshold detector/activator 24 with the dynamic transpositional gain controller output directed to the amplifier 20, in parallel with and summing together with the output of the dynamic harmonics controller 27 b. Alternatively, the transpositional gain controller 29, may operate as a real-time dynamic transpositional gain controller with its real-time activation triggered by the dynamic real-time gain filter 25 b with control signals in series, but with the transpositional gain controller 29 output being in parallel in one example of the loudspeaker system, and optionally in series in other examples.

FIG. 24 shows gain magnitude vs. frequency graph 30 n, illustrating three of the main gain filter shapes used in examples of the loudspeaker system with signal processing. Reference amplitude response curve 130 is shown without any gain filters applied. Gain filter curve 132 shows a narrowband gain filter shape, gain filter curve 134 shows a high-pass gain filter shape, and gain filter curve 136 shows a shelving gain filter shape. These filter shapes show one gain reduction curve for each filter shape, which could represent a fixed filter response, or just one gain reduction curve of a dynamic gain filter that may exhibit many different gain level curves of each of the curve shapes. These curve shapes can also be used either individually or combined to realize a more complex curve shape.

Referring to FIG. 25, shown is loudspeaker system 10 i with a signal processor 22 for enhancing low frequency output capability showing another example of the concept disclosed in other examples herein with signal processor 22 organized to illustrate a framework of example combinations of operational signal process options that accomplish the effecting principles of the loudspeaker system with signal processor, provides a system for minimizing audible overload distortion while increasing perceived low frequency output capability. The example system is comprised of at least one loudspeaker enclosure 12 b including at least one low frequency resonant chamber 16 and at least one electro-acoustical transducer 18 with a vibratile diaphragm 64 for converting an input electrical signal into a corresponding acoustic output signal. The resonant chamber 16 consists of at least one of a bass-reflex resonant chamber and a wave-resonant air-column chamber, which in this example is bass-reflex resonant chamber with vent 14 c. The enclosure 12 b also includes sealed, acoustic suspension chamber 13. Other example enclosures with a resonant chamber, such as disclosed herein, may be used with this example loudspeaker system. Also included is amplifier 20 and amplifier output/loudspeaker input 21 a and electrical signal input 23.

Referring also to FIG. 5, the loudspeaker system has a first frequency range 32 with a reduced diaphragm displacement and a fundamental resonant chamber 16 a resonance frequency F_(RC1) 34 at which a displacement characteristic of the vibratile diaphragm as a function of frequency has a minimum 34 a.

The example loudspeaker system 10 i has a second frequency range 36 adjacent to, and higher in frequency than, the first frequency range 32, including an increased diaphragm displacement and a frequency F_(MAX1) 37 a at which the displacement characteristic of the vibratile diaphragm as a function of frequency, above the resonant chamber resonance frequency 34, has a maximum. The loudspeaker system 10 i further has a third frequency range 39 above the frequency F_(MAX1) and a fourth frequency range 40 adjacent to, and lower in frequency than, the first frequency range, including an increased diaphragm displacement and a frequency F_(MAX2) 37 b at which the displacement characteristic of the vibratile diaphragm as a function of frequency, below the resonant chamber resonance frequency 34, reaches a maximum.

The loudspeaker 12 b and signal processor 22 includes at least one mode of the multi-mode processor 22, the mode being a filter gain controller 25 a for adjusting a gain of at least one gain adjusted frequency range, the at least one gain adjusted frequency range being at least one of the second frequency range 36 and the fourth frequency range 40, wherein, each gain filter is one of a narrowband filter 25 b and a high-pass filter 25 c, and each gain filter is also one of a fixed gain filter and a dynamic gain filter activated by the threshold detector/dynamic activator 24 b. At least one additional mode of the multi-mode signal processor 22 for providing at least a portion of a perceived replacement gain inversely corresponding to a reduced gain in the at least one gain adjusted frequency range, with the additional mode being one of a harmonics controller 27 a configured for controlling harmonics to create virtual fundamental frequency gain in the at least one gain adjusted frequency range or a transpositional gain controller 29 a to transpose a reduced gain from the at least one gain adjusted frequency range to an increased gain in the first frequency range.

Still further, the loudspeaker system and signal processor may include a threshold detector/dynamic activator 24 b configured to detect an audio amplitude threshold corresponding to a displacement level of the transducer 18 diaphragm 64 within a gain adjusted frequency range, which may be detected by way of feedback line 21 from amplifier 20 output 21 a, or it may be predictively determined from an audio signal at input 23 based on system gain profiles, wherein, at least one gain filter is a dynamic gain filter, and, when a predetermined transducer amplitude threshold is exceeded, the dynamic gain filter is activated, and as a level of an audio input signal within the gain adjusted frequency range is increased further, the gain of the dynamic gain filter is reduced in the gain adjusted frequency range. In this example of the loudspeaker system and signal processor, optionally, the threshold detector/dynamic activator 24 b upon the amplitude threshold being exceeded, can dynamically activate one or both of the narrowband filter 25 b and high-pass filter 25 c, which are optional portions of the filter gain controller block 25 a. The threshold detector/dynamic activator 24 b also may optionally dynamically activate one or both of the harmonics controller 27 a and the transpositional gain controller 29 a. Upon this dynamic activation, the gain filter can reduce gain in one or both of the second frequency range or the fourth frequency range to avoid an audible overload distortion and one or both of the harmonics generator and transpositional gain controller may provide at least a portion of replacement gain for any gain reduction of the frequency range 36 or frequency range 40, with the harmonics generator providing the replacement tonal gain as a virtual tonal gain derived from harmonics generated that correspond to the gain reduced fundamental frequencies in the gain reduced frequency ranges. The transpositional gain controller can replace reduced gain in the gain reduced frequency ranges by transposing at least a portion of the reduced gain as an additional gain in the displacement reduced frequency range 32, and preferably at resonance frequency and displacement minimum frequency 34/34 a. The dynamic activator will reduce gain in the dynamic gain filter and the additional mode of the multi-mode processor 22 of a harmonics controller/generator 27 a and/or transpositional gain controller will increase replacement gain in an inverse gain relationship to the dynamic gain filter.

As with other examples of the loudspeaker system and signal processor illustrated herein, the high excursion frequency ranges, such as frequency range 36 and frequency range 40, are reduced in level or gain by the filter gain controller 25 a, such as including the introduction of including one or more optional control blocks, pre-equalizer 80, narrowband filter 25 b, high pass filter 25 c and shelving filter 25 d to minimize audible overload distortion while additional modes of the multi-modal signal processor 22, such as harmonics controller/generator 27 a and transpositional gain controller 29 a are applied to substantially restore a perceived tonal and physical impact to a perceptual correspondence with a reference or target frequency response, such as 35 b in FIG. 2. These processes may be made dynamic by the processing modes of a threshold detector/dynamic activator 24 b to activate at least one of the filter gain controller harmonics controller/generator 27 a, or transpositional gain controller 29 a upon exceeding a predetermined transducer amplitude threshold. Operationally, the dynamic processing includes a substantially instant, real-time gain reduction onset time, and may have a delayed gain recovery time, or a real-time gain recovery. It may be preferred that the gain onset and recovery times of interacting processes, such as dynamic filter gain control, dynamic harmonics control and transpositional gain control, substantially match between the interacting processes so as to have a perceived tonal and physical gain replacement maintain perceptual correspondence with a predetermined reference or target frequency response curve. An additional aspect of the loudspeaker system and signal processor is to have the affect of the filter gain controller 25 a gain reductions of either frequency range 36 or frequency range 40 have little impact on the frequency range 32 so as to substantially maintain the level of frequency range 32 to sustain a perceived tonal and physical impact level.

It may be aurally advantageous in some examples of the loudspeaker system and signal processor, upon invoking a harmonics controller/generator 27 a to create a virtual gain in a gain reduced frequency range, or invoking the transpositional gain controller 29 a to produce a replacement gain in frequency range 32 to replace a gain reduced frequency range, to also further minimize the gain in the gain reduced frequency range so as to not have the actual fundamental frequencies in the gain reduced frequency ranges perceptually interfere with the replacement gain processes. This, among a number of other interactive processes may be empirically gain balanced to create the most affective perceptual fidelity.

Additionally the loudspeaker and signal processor may be most effective when optimizing the resonant chamber enclosure alignment by incorporating a set of transducer and enclosure parameters to be configured for a resulting frequency spacing ratio F_(SR1)=F_(MAX1)/F_(RC1) such that a value of F_(SR1) is between 1.2 and 2.9, or between 1.3 and 2.6, or between 1.43 and 2.3.

With the examples of the loudspeaker system with signal processor disclosed and other examples of the loudspeaker system, the dynamic harmonics generator 27, and/or the dynamic transpositional gain controller 29 may be used to not only replace the tonal and impact gain of the frequencies that are gain reduced by a dynamic gain filter, such as a dynamic narrowband filter, but to also increase the gain even more on peaks, such that the dynamic range of the bass in not only effective at maintaining fidelity at large signal levels, but to go beyond that to increase the perceived dynamic range of the system, operating as a bass dynamic range expander.

The operation of each block of the signal processing block may be configured and operated in a manner known to those practiced in the signal processing art, particularly dynamic equalization, virtual bass harmonics, may be created by creating a side chain signal path and clipping the portion of the input signal appearing in that side chain for which the fundamental frequencies that are clipped, symmetrically or asymmetrically, and optimized to create even, odd, or even and odd harmonics, and to create harmonics associated with those frequencies wherein those harmonics may be shaped by a filter, as example a low pass filter. By creating a narrowband filter to capture the frequency range that is gain reduced by the dynamic narrowband filter, one may utilize the clipping of that narrowband of frequencies of the input signal to create the appropriate range of harmonics to ‘recreate’ the perception of the gain reduced fundamentals. The harmonics generated may preferably be the even harmonics, the odd harmonics or a mix of even and odd harmonics of the fundamental frequencies within the gain reduced range.

Referring again to FIG. 1 and FIG. 3, the dynamic narrowband filter 25 represented by the narrow gain suppression band 36 has a number of advantages when matched to the resonant air chamber loudspeaker 12.

One of the advantages of the dynamic narrowband filter may have a more flexible variety of onset/attack and decay times. The onset/attack time is substantially real-time and instantaneous and the decay or release time may be much longer, associated with a timeframe approximating the cycle time of the lowest frequency being dynamically gain adapted. An advantage of the current loudspeaker system and signal processor with its dynamic narrowband filter, at the second frequency band, as with bandwidth 36 in FIG. 3, is that the dynamic narrowband filter has a higher frequency of operation that of a dynamic equalizer broad high pass filter, and then the decay time of the invention can be substantially shorter in duration while avoiding audible pumping and distortion. Alternatively, the dynamic narrowband filter of the current loudspeaker system and signal processor can operate with substantially instantaneous, real-time attack and decay times, or effectively real-time limiting the narrowband 36 of FIG. 3, above the unclipped first band, 32 of FIG. 3.

Having the gain of the gain reduced frequencies of 36 of FIG. 3 transposed to F_(RC1) 34 may be achieved by a number of means, including the use of full wave rectification to derive the absolute value of the gain reduction of the gain reduced frequencies to establish the amount of gain to transpose to F_(RC1) 34 when the range 36 exceeds the threshold to activate gain reduction of frequency range 36 or frequency range 40.

In examples of the current loudspeaker system and signal processor, particularly as in first example 10 a, a first harmonics generation is created on a dynamic basis, wherein at low, sub-threshold levels there are no harmonics generated and the harmonics are activated only when the signal exceeds the predetermined threshold, and then harmonics are gain increased in coordination with the gain reduction of the dynamic narrowband filter, creating a non-linear relationship with the input signal gain. This has multiple benefits over a fixed or linear harmonics generator that operates with full virtual pitch harmonics gain at all signal levels of the bass. By using a non-linear harmonics generation that only fills in for ‘reduced gain fundamentals’, rather than totally ‘missing fundamentals’, and because in one example harmonics generator of the current loudspeaker system and signal processor may be engaged fully when bass levels reach a predetermined threshold, the natural fundamentals at low or average levels may support the maintenance of a more natural, realistic perception of sound quality by requiring less harmonics generation enhancement to create the full perceived level of bass in the gain reduced frequency band, 36, as excess harmonics generation of ‘missing fundamentals’ can cause greater audible coloration and distortion of the sound quality.

In another preferred embodiment of the current loudspeaker system and signal processor, transposition of gain reduced frequencies to F_(RC1) 34 may also be created on a dynamic basis, wherein at low levels there may be no transposition of frequencies and gain of those frequencies, and the transposition may be fully activated when the signal exceeds the predetermined threshold, and then harmonics are gain increased by the dynamic harmonics generator 27 in coordination with the gain reduction of the dynamic narrowband filter 25, creating a non-linear relationship with the input signal gain. It is important that any transposed frequency have a dynamic filter gain or harmonics generation supporting the fidelity of the transpositional gain controller and the singular transposition frequency (preferably at or near F_(RC1) 34) to maintain the perception of a high fidelity tonality to the original input signal, and with frequency gaps in the sound with one frequency (transpositional frequency) may stand out and be audibly perceived as not harmonically related to the audio program signal. As the actual fundamental frequencies are transposed to a processor generated frequency F_(RC1) 34 which in most of the loudspeaker system and signal processor examples isn't related to the input signal (not a frequency derived from the audio program material), dynamic gain of frequencies from the dynamic harmonics generator may be important to create a convincing harmonic structure and pitch that corresponds to the audio input signal, even if it isn't the same as the audio input signal. While the ear/brain system is less and less pitch sensitive as the frequency range falls below 100 Hz and even more so below 70 Hz. The reduced pitch sensitivity, combined with pitch enhancement from the dynamic harmonics generator may allow the loudspeaker system and signal processor to maintain an effective tonal and physical perceptual replication of a large, high output, non-signal processed system.

An additional novel aspect of the loudspeaker system and signal processor that can be incorporated is to have any one or more of the dynamic narrowband filter, dynamic harmonics generator, and transpositional gain controller have a phase lead or time delay relative to the other process or processes.

Referring to graph 30 a in FIG. 3, for frequencies below first frequency range 32, at least a portion of the fundamental frequencies that are gain reduced by the fixed high pass filter, shown as an example curve 40 b may have an additional harmonics generation process for creating harmonics that correspond to the gain reduced fundamentals 40 b. For this additional, or fourth, frequency range 40, there may be a fixed harmonics generating process, or a dynamic harmonics generator.

It is an additional feature of the loudspeaker system and signal processor that the loudspeaker enclosure reproducing the harmonics generated by the dynamic harmonics generator 27 may be the same as the enclosure receiving the dynamic narrowband filter processing or the harmonics may be reproduced by a separate enclosure and transducer, from the same channel or from a different channel of a multi-channel audio system, such as, but not limited to, a smaller upper range loudspeaker operating in a range above the lower frequency bass, woofer or subwoofer system.

The signal processes in signal processor block 22 of analog or digital hardware, or software based or some mix of one or more of the three.

Referencing FIG. 1 and FIG. 3, the current loudspeaker system and signal processor, the example includes primary system and processes wherein gain is substantially maintained in a first frequency range and the processor 22 includes a threshold detector 24, for first detecting a threshold level relative to the second frequency band 36, the dynamic narrowband filter 25 for first, upon the threshold being exceeded, reducing gain in second frequency band 36, a dynamic harmonics generator 27 for generating harmonics predominantly above frequency band 36 that correspond to gain reduced frequencies within frequency band 36, to allow total system gain to increase beyond the threshold while protecting the transducer from one of an displacement overload and a thermal overload. In addition to this primary system and process, a number of secondary complimentary attributes may be included or added in certain preferred examples of the current loudspeaker system and signal processor, including; a fixed pre-equalization to optimize the small signal starting frequency balance of the system, a gain control system operating below the first frequency range 32, in frequency range 40, including a fixed amplitude suppression curve, such as example curve high pass filter 40 b or a fixed narrowband filter 40 c, or a dynamic high pass equalizer with an example curve 40 d in FIG. 5 or secondary dynamic narrowband (or notch) gain filter with one example curve shown as 40 e in FIG. 5, a fixed or dynamic harmonics generator corresponding to fundamental frequencies in frequency band 40 or other beneficial frequency or amplitude modifications that compliment the primary system and processes.

Additionally, the dynamic gain filters may also incorporate increased gain, or gain increasing ability, in combination with gain reducing ability, to offer a bass boost or correct for an amplitude depression within the operating range of the system.

Throughout the specification, the term ‘fundamental frequencies’ is most often referring to frequencies that are the fundamentals in relationship to the generated harmonics, e.g. those generated harmonics are harmonics of the fundamental, wherein the fundamentals may be gain reduced, frequencies. “Fundamental” may also refer to a fundamental resonant chamber resonance frequency, being the first or lowest frequency resonance frequency of a series of resonant chamber resonance frequencies.

Referring now to FIG. 6 and FIG. 7 the dynamic transpositional gain controller 29 as one example of operation, may, for purposes of understanding, be viewed as a dynamic gain/amplitude carrier frequency, or a specific frequency gain generator, at or near resonant chamber resonance frequency F_(RC1) 34 that operates at the carrier frequency rate, but adopts and accumulates corresponding gain from the gain reduced frequencies as shown in an example curve 36 b of band 36 and optionally the gain reduced frequencies show as example curve 42 b of band 42. In one preferred embodiment the transpositional carrier is substantially dormant at small signal levels and activated upon a predetermined threshold, and above such threshold, transpose gain reduced frequencies shown in one example curve 36 b from frequency range 36 and/or gain reduced frequencies 42 b from frequency range 42, while using the transpositional frequency 34 to represent the acoustic energy from the gain reduced bands and also engage the transpositional frequency, and as an option, in addition frequencies near transpositional frequency 34, as shown in first frequency band 32, to reproduce the audio input frequencies that fall into frequency band 32. Alternatively, above the predetermined threshold and all frequencies in frequency band 36 and below frequency band 36 of FIG. 7 may be transposed and gain represented by transpositional frequency 34.

As a guideline, transpositional frequency 34 may be equal to air-chamber resonant frequency F_(RC1), but in practical applications, the transpositional frequency 34 may vary somewhat from air-chamber resonant frequency F_(RC1), due to systems design tolerances, variation over time, drift, or a design or performance preference. This variation away from precisely F_(RC1) would tend to be on the order of plus and minus less than approximately 10% frequency change from F_(RC1). This would be in keeping with staying substantially centered within the frequency range 32 in FIG. 3, which is a displacement minimized frequency range.

In examples of the loudspeaker system and signal processor, the level based threshold may be most effective sensed or derived by sampling at a point in the signal path at least after a volume control and volume control setting, and preferably after an amplifier output. Alternatively the gain profiles of the electronic signal path may be known and allow a predictive threshold detector.

Referring to FIG. 1 and FIG. 3, the threshold detector/activator 24 may be based on a threshold curve that substantially corresponds to the diaphragm displacement curve, for example the graph of the diaphragm displacement curve 30 a portion 36 a shown in frequency band 36, with displacement maximum 37 a and optionally frequency band 40 with displacement maximum 37 b.

As the current loudspeaker system and signal processor reduces the gain of the higher displacement frequency bands, such as band 36 and band 40 in graph 30 a in FIG. 3, and allows system gain to continue to increase at tuning frequency F_(RC1) 34 and frequencies above band 36, the inventive system can provide substantially increased output capability without displacement overload of the transducer 18, eventually as the program volume is increased and gain increase at, or near, frequency F_(RC1) 34 to the point where even at that displacement minimum, the displacement begins to exceed the maximum linear displacement capability of the transducer 18, a final threshold may be deployed which in addition to the narrow band gain reductions that have been imposed by the dynamic narrowband filter, an additional broader band dynamic high pass gain filter may begin to gain reduce the gain applied to the transducer 18 from a frequency as high as somewhat above frequency band 36 all the way down to the lowest frequency portion of frequency band 40, substantially keeping the transducer from being audibly overloaded. The dynamic harmonics generator 27 can be further coordinated with this broad band high pass dynamic gain filter by generating additional harmonics in the frequency range above the upper half of frequency range 36 with the generated harmonics corresponding to at least a portion of the gain reduced fundamentals being gain reduced by the dynamic high pass gain filter.

Another technology that can be effectively integrated into the examples of the loudspeaker system and signal processor, as a further enhancement, is that of a haptics or tactile transducer to further stimulating the sensation of physical bass impact. As the predetermined threshold of the threshold detector/activator 24 is exceeded, in addition to the other signal processes being engaged, as discussed above, the tactile transducer can be activated and gain increased correspondingly to the gain reduction of the dynamic gain reduction processes and the gain increase of the program material. Alternatively, a frequency of reduced level or gain reduction may have at least a portion of that level or gain transposed to a frequency of operation in a tactile transducer or haptic device, wherein those devices would be utilized to enhance a perceived physical impact.

In an example of the loudspeaker system and signal processor, it can be useful to incorporate at least a portion of or all of, the starting fixed target equalization into the dynamic gain filter, or the dynamic narrowband filter, as the target equalization established below the amplitude threshold level.

Dynamic gain filters, including the dynamic narrowband filter, may have a positive gain in there operational frequency range, such as the second frequency range or the fourth frequency range, or any dynamically gain reduced frequency range.

It contributes to perceived physical impact to maintain the gain in the gain reduced frequency range 32 above the gain reduced gain levels in a gain reduced frequency range.

Besides the application to small systems, the current loudspeaker system and signal processor can provide significant dynamic enhancement to larger-scale loudspeaker systems such as used in professional sound reinforcement systems and consumer audio systems, in that many of them are sound pressure level limited by the narrow band of frequencies such as the frequency band 36 in FIG. 3. By applying the processing and structures of the examples of the loudspeaker system with signal processing, these large scale systems can be enhanced to increase their apparent low frequency output by approximately six decibels or more, which is four times the power or more and can allow the use of half the number of bass speakers which may be very useful in providing more output from a system of reduced size and cost.

Applying the inventive loudspeaker enclosure signal processing system can be effective for, most any small or large electro-acoustic system, such as cell phones, small multi-media systems, stereo and surround sound systems, professional sound reinforcement systems, subwoofers, portable systems and most any other audio system of one or more channels, for increasing the apparent low frequency capability and dynamic range of the loudspeaker system.

In any of the example systems the signal processor 22 may be applied to further enhance the dynamic range of the low frequency system of the loudspeaker system by operating dynamically as a low frequency dynamic range expander, with non-linear expansion of low frequency signal gain.

When transpositional frequency target, the first frequency range can be as little as little as a quarter-octave or less in bandwidth. The threshold can be determined from a predictive analysis of the input signal or from a feedback signal from at least one of the output 21 a of the amplifier 20, a sensor on the transducer, and a sensor at the output of the transducer. The threshold can be derived from at least one of an onset of diaphragm 64 displacement, amplifier 20 overload and/or a voice coil thermal limit.

In the example loudspeaker system and signal processing includes at least two of a gain filter, a harmonics generator, and a transpositional gain controller, wherein the gain filter is at least one of a narrowband gain filter and a high-pass filter. It is desirable that the low displacement frequency range 32 is substantially maintained at a signal level or gain level when level or gain is reduced in second frequency range 36 or fourth frequency range 40.

Some, or all, of the signal processes of signal processor 22 may be accomplished by processing with one or more of software or hardware, analog or digital circuitry. The processing may also arranged to process downloaded program material, or program material stored an online or cloud storage medium or any storage medium. At least a portion of the disclosed processing may also be applied as a preprocess to program material, and may be dedicated to a particular loudspeaker type or specification, and may be a process that program material can be uploaded to a location and processed with the inventive processing and returned to a user or distributor of the program material. Program material from any source may be processed and returned to a storage medium in processed form with at least a portion of the disclosed processing steps.

It is evident that those skilled in the art may now make numerous uses of and departures from the specific apparatus and techniques disclosed herein without departing from the inventive concepts. Consequently, the current loudspeaker system and signal processor invention is to be construed as embracing each and every novel feature and novel combination of features disclosed herein, and the examples of the present invention disclosed herein are intended to be illustrative, but not limiting, of the scope of the invention

Finally, it should be noted that the language used in the specification has been principally selected for readability and instructional purposes, and may not have been selected to delineate or circumscribe the inventive subject matter. Accordingly, the disclosure of the present loudspeaker system and signal processor invention is intended to be illustrative, but not limiting, of the scope of the invention. 

What is claimed is:
 1. A loudspeaker system including a multi-mode signal processor for minimizing audible overload distortion while increasing perceived low frequency output capability, comprising; at least one loudspeaker enclosure including at least one low frequency resonant chamber and at least one electro-acoustical transducer with a vibratile diaphragm for converting an input audio electrical signal into a corresponding acoustic output signal, with the resonant chamber consisting of at least one of a bass-reflex resonant chamber and a wave-resonant air-column chamber, a first frequency range with a reduced diaphragm displacement and a fundamental resonant chamber resonance frequency F_(RC1) at which a displacement characteristic of the vibratile diaphragm as a function of frequency has a minimum, a second frequency range adjacent to, and higher in frequency than, the first frequency range including an increased diaphragm displacement and a frequency F_(MAX1) at which the displacement characteristic of the vibratile diaphragm as a function of frequency above the resonant chamber resonance frequency has a maximum, a third frequency range above the frequency F_(MAX1), a primary dynamic narrowband filter for dynamically adjusting a gain of one or more frequencies within the second frequency range, a harmonics controller, incorporating a dynamic harmonics generator, to dynamically generate harmonics in the third frequency range creating a virtual fundamental tonal gain in the second frequency range that corresponds to the dynamically gain adjusted frequencies in the second frequency range and creating at least a partial tonal gain replacement for the gain reduced frequencies in the second frequency range, a threshold detector configured to detect a primary narrowband audio amplitude threshold corresponding to a displacement of the transducer diaphragm within the second frequency range, wherein when an audio signal level is below the primary narrowband amplitude threshold the primary dynamic narrowband filter is inactive, and when the primary narrowband audio amplitude threshold is exceeded, the primary dynamic narrowband filter is activated and the dynamic harmonics generator is cooperatively activated with the dynamic narrowband filter, and as a level of an audio input signal within the second frequency range is increased further, the gain of the primary dynamic narrowband filter is reduced and the harmonics gain of the dynamic harmonics generator is increased, and, when operating above the primary narrowband amplitude threshold the signal processor operates with the dynamic narrowband filter gain and the dynamic harmonics generator gain corresponding in an inverse relationship to each other, and as the filter gain in the second frequency band is dynamically reduced to minimize an audible overload distortion, a first frequency range acoustic level is substantially maintained relative to that of an acoustic level of the second frequency range, to more effectively maintain a perceived physical bass impact, and the harmonics gain in the third frequency range is increased to more effectively maintain a perception of a tonal level in the second frequency range.
 2. The loudspeaker system of claim 1, wherein a combined set of transducer and enclosure parameters are configured for a frequency spacing ratio F_(SR1)=F_(MAX1)/F_(RC1) such that a value of F_(SR1) is between 1.2 and 2.9.
 3. The loudspeaker system of claim 1, wherein a combined set of transducer and enclosure parameters are configured for a frequency spacing ratio F_(SR1)=F_(MAX1)/F_(RC1) such that a value of F_(SR1) is between 1.3 and 2.6.
 4. The loudspeaker system of claim 1, wherein a combined set of transducer and enclosure parameters are configured for a frequency spacing ratio F_(SR1)=F_(MAX1)/F_(RC1) such that a value of F_(SR1) is between 1.43 and 2.3.
 5. The loudspeaker system of claim 1, wherein when an audio signal level is below the primary narrowband amplitude threshold the primary dynamic harmonics generator is inactive.
 6. The loudspeaker system of claim 1, further comprising; a fourth frequency range of frequencies below the fundamental resonant chamber resonance frequency with a fixed gain filter operating in the fourth frequency range, the fixed gain filter being at least one of a high-pass filter and a narrowband filter for reducing a gain of frequencies in the fourth frequency range.
 7. The loudspeaker system of claim 1, further comprising; a fourth frequency range of frequencies, below the fundamental resonant chamber resonance, with a fixed gain filter operating in the fourth frequency range, the fixed gain reduction filter being at least one of a high-pass filter and a narrowband filter for reducing a gain of frequencies in the fourth frequency range, the harmonics generator further configured to generate harmonics corresponding to gain reduced frequencies in the fourth frequency range.
 8. The loudspeaker system of claim 1, further comprising; a fourth frequency range of frequencies below the fundamental resonant chamber resonance frequency, with a dynamic gain filter operating in the fourth frequency range, the dynamic gain filter being at least one of a high-pass filter and a narrowband filter, the threshold detector configured to detect a secondary audio amplitude threshold corresponding to a displacement of the transducer diaphragm within the fourth frequency range, the dynamic gain filter activated for a secondary gain reduction within the fourth frequency range when the threshold detector exceeds the secondary amplitude threshold.
 9. The loudspeaker system of claim 1, further comprising; a fourth frequency range of frequencies below the fundamental resonant chamber resonance frequency, with a dynamic gain filter operating in the fourth frequency range, wherein, the dynamic gain filter configured to include at least one of a high-pass filter and a narrowband filter, the threshold detector is configured to detect a secondary audio amplitude threshold corresponding to a displacement of the transducer diaphragm within the fourth frequency range, and the dynamic gain filter activated for a secondary gain reduction within the fourth frequency range when an amplitude level in the fourth frequency range exceeds the secondary amplitude threshold, the harmonics generator further configured as a secondary dynamic harmonics generator producing harmonics and dynamically adjusting a harmonics gain with the produced harmonics and the harmonics gain corresponding inversely to the dynamically gain adjusted frequencies within the fourth frequency range.
 10. The loudspeaker system of claim 1, further comprising a transpositional gain controller, the transpositional gain controller incorporating a dynamic transpositional gain controller, wherein, when the loudspeaker system is operating above the primary narrowband amplitude threshold and the gain in the second frequency range is reduced by the primary dynamic narrowband filter, a magnitude of a gain corresponding to at least a portion of the gain reduction of a frequency of the input audio electrical signal within the second frequency range is dynamically transposed as an additional gain at a frequency of reduced diaphragm displacement within the first frequency range, when operating above the primary narrowband amplitude threshold the signal processor operates with the dynamic narrowband filter gain and the dynamic transpositional gain controller gain corresponding in an inverse relationship to each other, the dynamic transpositional gain replacing at least a portion of the reduced gain in the second frequency range to replace at least a portion of a physical impact removed from the second frequency range and more effectively maintain the perceived physical bass impact.
 11. The loudspeaker system of claim 1, further comprising a transpositional gain controller, and; the transpositional gain controller incorporating a dynamic transpositional gain controller with a signal generator for generating a variable gain signal at a frequency of reduced diaphragm displacement within the first frequency range, wherein; when the loudspeaker system is operating above the primary narrowband amplitude threshold and the gain in the second frequency range is reduced by the primary dynamic narrowband filter, a magnitude of a gain corresponding to at least a portion of the gain reduction of a frequency of the input audio electrical signal within the second frequency range is dynamically transposed as an additional gain at the frequency of reduced diaphragm displacement within the first frequency range, when operating above the primary narrowband amplitude threshold the signal processor operates with the dynamic narrowband filter gain and the dynamic transpositional gain controller gain corresponding in an inverse relationship to each other, the dynamic transpositional gain replacing at least a portion of the reduced gain in the second frequency range to replace a least a portion of a physical impact removed from the second frequency range and more effectively maintain the perceived physical bass impact.
 12. The loudspeaker system of claim 10, wherein when the loudspeaker system is operating below the primary narrowband amplitude threshold, the dynamic transpositional gain controller is inactive.
 13. The loudspeaker system of claim 10, wherein the frequency of reduced diaphragm displacement is the fundamental resonant chamber resonance frequency plus or minus less than a ten percent component tolerance.
 14. The loudspeaker system of claim 11, wherein the frequency of reduced diaphragm displacement is the fundamental resonant chamber resonance frequency plus or minus less than a ten percent component tolerance.
 15. The loudspeaker system of claim 10, wherein the dynamically transposed gain replacing a physical bass impact of the reduced gain of the second frequency range and the dynamic harmonics gain replacing the a tonal level of the reduced gain of the second frequency range, are balanced in a gain level to provide a perception of tonal level and physical bass impact level substantially matching the physical impact and tonal quality of a frequency response without a gain reduction in the second frequency range.
 16. The loudspeaker system of claim 11, wherein the dynamically transposed gain replacing a physical bass impact of the reduced gain of the second frequency range and the dynamic harmonics gain replacing the a tonal level of the reduced gain of the second frequency range, are balanced in a gain level to provide a perception of tonal level and physical bass impact level substantially matching the physical impact and tonal quality of a frequency response without a gain reduction in the second frequency range.
 17. The loudspeaker system of claim 1, wherein the dynamic narrowband filter has a gain reduction attack-time and a gain recovery release-time, with the gain recovery release-time being longer than the gain reduction attack-time.
 18. The loudspeaker system of claim 1, wherein the dynamic narrowband filter is a real-time dynamic filter and has a gain reduction attack-time and a gain recovery release-time that are both essentially instantaneous.
 19. The loudspeaker system of claim 18, wherein the harmonics controller controls a real-time attack time and release time distortion by at least one of shaping, cancelling and adding to, a harmonic distortion produced by the real-time dynamic narrowband filter.
 20. The loudspeaker system of claim 1, wherein the dynamic narrowband filter is an incremental gain change filter.
 21. The loudspeaker system of claim 1, wherein the dynamic narrowband filter is a gain step gain change filter.
 22. The loudspeaker system of claim 11, wherein when the loudspeaker system is operating below the primary narrowband amplitude threshold, the dynamic transpositional gain controller is inactive.
 23. A loudspeaker system including a multi-mode signal processor for minimizing audible overload distortion while increasing perceived low frequency output capability, comprising; at least one loudspeaker enclosure including at least one low frequency resonant chamber and at least one electro-acoustical transducer with a vibratile diaphragm for converting an input electrical signal into a corresponding acoustic output signal, with the resonant chamber consisting of at least one of a bass-reflex resonant chamber and a wave-resonant air-column chamber, a first frequency range with a reduced diaphragm displacement including a fundamental resonant chamber resonance frequency F_(RC1) at which a displacement characteristic of the vibratile diaphragm as a function of frequency has a minimum, a second frequency range adjacent to, and higher in frequency than the first frequency range, including an increased diaphragm displacement and a frequency F_(MAX1) at which the displacement characteristic of the vibratile diaphragm as a function of frequency, above the fundamental resonant chamber resonance frequency, has a maximum, a third frequency range above the frequency F_(MAX1), a fourth frequency range adjacent to, and lower in frequency than the first frequency range, including an increased diaphragm displacement and a frequency F_(MAX2) at which the displacement characteristic of the vibratile diaphragm as a function of frequency, below the fundamental resonant chamber resonance frequency, reaches a maximum, at least one gain filter mode for adjusting a gain of at least one gain adjusted frequency range, the at least one gain adjusted frequency range being at least one of the second frequency range and the fourth frequency range, wherein, each gain filter is one of a narrowband filter and a high-pass filter, and each gain filter is one of a fixed gain filter and a dynamic gain filter, at least one additional mode of the multi-mode signal processor for providing at least a portion of a perceived replacement gain inversely corresponding to a reduced gain in the at least one gain adjusted frequency range, the additional mode being one of a harmonics controller configured for controlling harmonics to create virtual fundamental frequency gain in the at least one gain adjusted frequency range and a transpositional gain controller to transpose a reduced gain from the at least one gain adjusted frequency range to an increased gain in the first frequency range.
 24. The loudspeaker system of claim 23, wherein a combined set of transducer and enclosure parameters are configured for a frequency spacing ratio F_(SR1)=F_(MAX1)/F_(RC1) such that a value of F_(SR1) is between 1.2 and 2.9.
 25. The loudspeaker system of claim 23, wherein a combined set of transducer and enclosure parameters are configured for a frequency spacing ratio F_(SR1)=F_(MAX1)/F_(RC1) such that a value of F_(SR1) is preferably between 1.3 and 2.6.
 26. The loudspeaker system of claim 23, wherein a combined set of transducer and enclosure parameters are configured for a frequency spacing ratio F_(SR1)=F_(MAX1)/F_(RC1) such that a value of F_(SR1) is even more preferable between 1.43 and 2.3.
 27. The loudspeaker system of claim 23, further comprising a threshold detector configured to detect an audio amplitude threshold corresponding to a displacement level of the transducer diaphragm within the gain adjusted frequency range, wherein, one gain filter of the at least one gain filter is a dynamic gain filter, and, when the amplitude threshold is exceeded, the dynamic gain filter is activated, and as a level of an audio input signal within the gain adjusted frequency range is increased further, the gain of the dynamic gain filter is reduced in the gain adjusted frequency range.
 28. The loudspeaker system of claim 27, wherein the gain adjusted frequency range is the fourth frequency range.
 29. The loudspeaker system of claim 27, wherein the gain adjusted frequency range is the second frequency range and the dynamic gain filter is a narrowband gain filter.
 30. The loudspeaker system of claim 23, wherein the at least one additional mode of the multi-mode signal processor is the transpositional gain controller.
 31. The loudspeaker system of claim 23, wherein the at least one additional mode of the multi-mode signal processor is the harmonics controller.
 32. The loudspeaker system of claim 23, wherein the at least one additional mode of the multi-mode signal processor includes both the transpositional gain controller and the harmonics controller.
 33. The loudspeaker system of claim 27, wherein the dynamic gain filter has a gain reduction attack-time and a gain recovery release-time, with the gain recovery release-time being longer than the gain reduction attack-time.
 34. The loudspeaker system of claim 27, wherein the dynamic gain filter is a real-time dynamic filter and has a gain reduction attack-time and a gain recovery release-time that are both essentially instantaneous.
 35. The loudspeaker system of claim 34, wherein a harmonics controller controls a real-time attack time and release time distortion by at least one of shaping, cancelling and adding to, a harmonic distortion produced by the real-time dynamic gain filter.
 36. The loudspeaker system of claim 27, wherein the dynamic gain filter is an incremental gain change filter.
 37. The loudspeaker system of claim 27, wherein the dynamic gain filter is a gain stepped gain change filter with individual gain steps, wherein each gain step is at least 3 dB.
 38. The loudspeaker system of claim 31, wherein; the at least one loudspeaker enclosure is a first loudspeaker enclosure and the at least one transducer is a first transducer mounted in the first loudspeaker enclosure, wherein the loudspeaker system includes at least a second electro-acoustical transducer with a vibratile diaphragm for converting an input audio electrical signal into a corresponding acoustic output, wherein, the harmonics controller generates harmonics in an operational frequency range of the second transducer to create virtual fundamental frequency gain in the at least one gain adjusted frequency range.
 39. The loudspeaker system of claim 38, wherein; the second transducer is mounted to a second loudspeaker enclosure or baffle.
 40. The loudspeaker system of claim 38, wherein; the amplifier includes a first amplifier channel and the second transducer is connected to a second amplifier channel.
 41. The loudspeaker of claim 23, wherein; the at least one gain filter includes a fixed gain filter in the second frequency range and a fixed gain filter in the fourth frequency range, and the fixed band filter in the second frequency range is a narrowband filter, and the fixed band filter in the fourth frequency range is one of a high-pass filter and a narrowband filter.
 42. The loudspeaker of claim 41, wherein; the at least one additional mode of the multi-mode signal processor for providing at least a portion of a perceived replacement gain inversely corresponding to a reduced gain in the at least one gain adjusted frequency range, is both the harmonics controller and the transpositional gain controller.
 43. The loudspeaker system of claim 28, wherein; the loudspeaker enclosure includes a bass-reflex resonant chamber and an acoustic suspension sealed chamber.
 44. The loudspeaker system of claim 43, wherein; an additional gain adjusted frequency range is the second frequency range and the dynamic gain filter operating in the second frequency range is a narrowband gain filter.
 45. The loudspeaker system of claim 43, wherein; the second of the at least one additional mode of the multi-mode signal processor for providing at least a portion of a perceived replacement gain inversely corresponding to a reduced gain in the gain adjusted frequency range, is the transpositional gain controller.
 46. The loudspeaker system of claim 44, wherein; the second of the at least one additional mode of the multi-mode signal processor for providing at least a portion of a perceived replacement gain inversely corresponding to a reduced gain in both gain adjusted frequency ranges, is the transpositional gain controller.
 47. The loudspeaker system of claim 23, wherein; the transpositional gain controller transposes at least a portion of a gain, corresponding to a reduced level frequency range, to a frequency of operation of a tactile transducer.
 48. A method for minimizing audible overload distortion of a loudspeaker system and increasing a perceived low frequency output capability, incorporating an amplifier and at least one transducer with a vibratile diaphragm, and a low frequency signal processor, including the steps of; configuring a loudspeaker enclosure to include at least one resonant chamber providing a resonant chamber resonance frequency; identifying a first frequency range of reduced transducer diaphragm displacement including the fundamental resonant chamber resonance frequency at which a displacement characteristic of the vibratile diaphragm as a function of frequency has a minimum; identifying an increased diaphragm displacement frequency range adjacent to the first frequency range; establishing at least one amplitude threshold within the increased diaphragm displacement frequency range; configuring the signal processor to activate a dynamic gain filter for activating a dynamic gain reduction in the increased diaphragm displacement frequency range and for activating a dynamic harmonics generator for generating harmonics, the harmonics corresponding to gain reduced fundamental frequencies in the increased diaphragm displacement frequency range, when an audio signal, derived from an input signal, exceeds the at least one amplitude threshold; dynamically increasing a level of the generated harmonics in correspondence to the gain reduction of the gain reduced fundamental frequencies in increased diaphragm displacement frequency range.
 49. The method of claim 48 including the further step of; configuring the signal processor to substantially maintain a gain in the first frequency range when the gain in the increased diaphragm displacement frequency range is reduced.
 50. The method of claim 48 including the further step of; configuring the signal processor such that the dynamic gain filter and the dynamic harmonics generator are inactive when the loudspeaker system is operating below the at least one amplitude threshold.
 51. The method of claim 48 including the further step of; a magnitude of gain corresponding to the gain reduction of signal frequencies within the increased diaphragm displacement frequency range is transposed as additional gain to a frequency of reduced displacement within the first frequency range when the gain is reduced in the dynamic gain filter.
 52. The method of claim 48 including the further steps of; establishing a frequency generator with adaptive gain in a predetermined frequency of reduced displacement within the first frequency range; when the gain being reduced in the dynamic gain filter, a magnitude of gain corresponding to the gain reduction of signal frequencies within the increased diaphragm displacement frequency range is applied as additional gain to the frequency generator in the frequency of reduced displacement. 